Chapter 4: Large-scale atmosphere-ocean processes affecting climate

Authors

Coordinating Lead Authors:

Michael Sigmond, Environment and Climate Change Canada

Karen Smith, University of Toronto Scarborough

Lead Authors:

Russell Blackport, Environment and Climate Change Canada

Alex J. Cannon, Environment and Climate Change Canada

William Merryfield, Environment and Climate Change Canada 

Rachel H. White, University of British Columbia

Bin Yu, Environment and Climate Change Canada

Contributing Authors:

Asli Bese, Ouranos

Louis-Philippe Caron, Ouranos

Dae Il Jeong, Environment and Climate Change Canada

Ruping Mo, Environment and Climate Change Canada

Acknowledgements

Zhenhua Li, University of Saskatchewan, for providing comments on a draft of Section 4.7

Wei Liu, University of California Riverside, for providing Figure 4.21b,c

Recommended chapter citation:

Sigmond, M., Smith, K.L., Blackport, R., Cannon, A.J., Merryfield, W.J., White, R.H., & Yu, B. (2026). Large-scale atmosphere-ocean processes affecting climate. In Canada’s Changing Climate Report 2026. (pp. xx–xx). Government of Canada.

Chapter description

This chapter assesses changes in processes and phenomena in the atmosphere and ocean that influence regional changes in Canadian climate, including Arctic amplification, atmosphere-ocean circulation patterns, and the large-scale conditions that lead to thunderstorms.

Chapter key messages

Key message 4.1

The Arctic (the region north of the Arctic circle) has warmed at more than three times the rate of the global average over the past five decades (high confidence). Most of this increased warming, known as Arctic amplification, is caused by human influence (high confidence) and involves local climate processes and feedbacks, including sea ice loss. It largely explains why Canada has warmed nearly twice as fast as the global average and the Canadian Arctic three times as fast for the period 1970-2023 (high confidence).

Key message 4.2

Arctic amplification, and the greater rate of warming in Canada’s Arctic compared to the rest of Canada, will continue over the 21st century (very high confidence). In the coming decades, the Canadian Arctic is projected to warm at more than twice the rate of the global average (medium confidence).

Key message 4.3

Changes in recent decades in the jet streams and storm tracks that affect Canada are small and seen only in limited seasons and regions. There is low confidence in any human influence on these past changes. An overall poleward shift in the jet streams and storm tracks is projected by the end of the 21st century, but the changes are small and depend on the region and season (low confidence).

Key message 4.4

Changes in recent decades in the frequency and intensity of extratropical storms and of atmospheric blocks are uncertain. There is low confidence in any human influence on these past changes. A poleward shift in extratropical storms and a decrease in the frequency of summer extratropical storms are projected over Canada (low confidence). Atmospheric blocks are projected to occur less frequently over Canada, but there are large regional variations (low confidence).

Key message 4.5

The frequency and intensity of atmospheric rivers have increased for Canada as a whole in recent decades (medium confidence). However, there is very low confidence in the magnitude of these increases due to the limited number of studies and the sensitivity of results to how atmospheric rivers are defined and detected. There is insufficient evidence to attribute long-term trends for Canada as a whole to human influence. However, human influence has increased the likelihood of extreme atmospheric-river events in southern British Columbia (low confidence). 

Key message4.6

The frequency and intensity of atmospheric rivers over Canada will increase in the future in high emissions scenarios (high confidence) and intermediate emissions scenarios (medium confidence). However, the magnitude of these increases is uncertain.

Key message 4.7

The strength and associated precipitation rates of North Atlantic hurricanes have increased (medium confidence). However, since only a small proportion of Atlantic hurricanes affect Canada, there is low confidence in the degree to which these changes have affected eastern Canada.

Key message 4.8

The average precipitation rates, maximum precipitation rates, and peak wind speeds associated with North Atlantic hurricanes, as well as the proportion of hurricanes in the North Atlantic that reach categories 4 and 5, are projected to increase (high confidence). However, regarding the small number of hurricanes affecting Canada, there is medium confidence in increasing precipitation rates and low confidence in increasing wind speeds. Changes in frequency of hurricanes affecting Canada are uncertain.  

Key message 4.9

There is low confidence that large-scale environmental conditions favouring thunderstorms in Canada have changed over the past several decades. This is due to a lack of regional studies for Canada, the weak, conflicting trends across different environmental-condition indicators and data products, and large internal climate variability.

Key message 4.10

Large-scale environmental conditions favouring thunderstorms are projected to become more prevalent across central and eastern Canada in spring, summer, and fall (high confidence). However, there is low confidence that thunderstorms and other severe weather events will increase, because an increase in favourable environmental conditions does not always lead to more thunderstorms.

Key message 4.11

The El Niño–Southern Oscillation (ENSO) is the dominant source of year-to-year climate variability in western Canada. Year-to-year climate fluctuations associated with ENSO have been larger since 1950 than in the previous century (medium confidence). However, there is low confidence that this change is due to human-caused climate change because internal climate variability is large.

Key message 4.12

The El Niño–Southern Oscillation (ENSO) will remain the dominant source of climate variability in western Canada in the 21st century (high confidence), but there is low confidence in projected changes in year-to-year climate fluctuations associated with ENSO. While climate models consistently show that by the end of the century, the effect of ENSO on winter climate fluctuations will extend into central and eastern Canada, there is low confidence in these projections due to systematic climate model biases.

Key message 4.13

The primary large-scale ocean current system affecting climate in Canada is the Atlantic Meridional Overturning Circulation (AMOC). A weaker than normal AMOC is associated with cooler and drier than normal winters over eastern Canada. There is high confidence that a temporary weakening of the AMOC between 2007 and 2015 led to a period of cooler North Atlantic Ocean surface temperatures and low confidence that this AMOC weakening can be attributed to human influence.

Key message 4.14

There is high confidence that the Atlantic Meridional Overturning Circulation (AMOC) will gradually weaken over the remainder of the 21st century due to human influence, and that this will slightly reduce the warming of eastern and northern Canada. However, the possibility that the AMOC could shut down, leading to a more pronounced regional cooling influence, cannot be ruled out. There is medium confidence that the AMOC will not shut down in the 21st century.

Key message 4.15

Changes that are due to thermodynamic processes are generally robust and well understood.

Key message 4.16

Regional variations in Canadian climate depend strongly on changes in dynamical processes, which are uncertain and less well understood.

Key message 4.17

There is generally more confidence in future human-caused changes than in the attribution of past changes to human-caused climate change.

Plain language summaryFootnote 1

In this chapter, we assess changes in processes and phenomena that influence regional changes in Canadian climate and are relevant to changes in surface temperature and precipitation (discussed in chapters 2 and 3) and in other variables (discussed in chapters 5 to 9). We distinguish between climate-related changes due to processes associated with changes in radiation and heat fluxes (thermodynamic processes) and those due to processes associated with the circulation of air in the atmosphere and water in the ocean (dynamical processes).

Thermodynamic processes are the main drivers of a phenomenon referred to as Arctic amplification, that is, the Arctic region’s faster increase in surface temperature compared to the global average surface temperature. This phenomenon largely explains why Canada has warmed at a faster rate than the global average, and why northern Canada has warmed at a faster rate than southern Canada, as reported in Chapter 2. Arctic amplification will continue to dominate global and Canadian warming patterns in the future. Thermodynamic processes are also associated with other projected changes. For example, the greater availability of water vapour in the atmosphere associated with global warming leads to an increase in the intensity and frequency of atmospheric rivers—long, narrow, corridors of strong horizontal water vapour transport in the atmosphere. Thermodynamic processes also contribute to the projected increase in environmental conditions that favour the development of thunderstorms, particularly across central and eastern Canada. In addition, we expect an increase in average and maximum rain rates associated with Atlantic hurricanes and in the proportion of Atlantic hurricanes that become very strong. However, since only a small number of Atlantic hurricanes affect Canada, uncertainty exists about how these changes will impact eastern Canada.

Changes in dynamical processes, such as in the large-scale circulation of air in the atmosphere, are important for understanding and predicting climate change in Canada at a regional level but are more uncertain than changes in thermodynamic processes. This uncertainty is due to the large impact of internal climate variability on dynamical processes and to the disagreement among models about many aspects of the projected changes. Changes in the large-scale atmospheric circulation are the result of large-scale variations in temperature. For example, Arctic amplification leads to a smaller difference in the near-surface temperature between the tropics and the Arctic. This generally contributes to a shift toward the equator in the location of the jet streams, strong bands of wind that flow from west to east throughout the lowest 15 km of the atmosphere (Figure 4.6). On the other hand, increased warming in the tropics’ upper troposphere, around 10 to 15 km above the Earth’s surface, tends to lead to a larger difference in the upper-level temperature between the tropics and the poles and contributes to a strengthening of the jet streams and their shift toward the poles. Climate models suggest that in most cases, the increased warming in the tropics will dominate, causing jet streams, extratropical storms, and atmospheric rivers to migrate toward the poles under climate change. An increase in the north-south meandering of the jet streams, making them wavier, and in the strength or frequency of atmospheric blocks (very slowly moving high pressure systems), could lead to more intense and more frequent climate extremes. However, there is no robust evidence that the waviness of the jet streams and strength or frequency of blocks have changed in the past or will do so in the future.

The El Niño–Southern Oscillation is a mode of variability characterized by fluctuations every two to seven years in sea surface temperatures and air pressure in the tropical Pacific Ocean. This mode of variability is also associated with large year-to-year fluctuations in Canadian climate. Currently limited mainly to western Canada, these fluctuations are projected to extend to central and eastern Canada in response to additional climate warming. However, these projections are uncertain due to systematic climate model biases in the tropical Pacific.

Future warming over eastern and northern Canada may be slightly reduced by a projected weakening of the Atlantic Meridional Overturning Circulation, the primary large-scale ocean current affecting Canadian climate, but the magnitude of this cooling influence is uncertain. A substantially larger cooling influence over eastern and northern Canada associated with a possible shutdown of this ocean current in this century cannot be ruled out.

4.1: Introduction

Chapters 2 and 3 provide detailed assessments of past and future average changes in temperature, precipitation, and surface winds, and a general overview of past and future changes in specific aspects of Canada’s climate based on the detailed assessments of those changes in chapters 4 to 9. This chapter is the first of those more technical chapters and describes and assesses changes in large-scale atmosphere and ocean processes that affect most other aspects of climate change in Canada discussed in other chapters. It assesses processes and phenomena that occur in the atmosphere and ocean on scales of more than 100 km, and that shape patterns of change in Canadian climate (figures 4.1, 4.3, Box 4.1). These large-scale processes explain why Canada is warming at a faster rate than the global average. They also contribute to spatial variations in temperature and precipitation changes in Canada, and to the other aspects of climate change in Canada described in chapters 5 to 9. For a more general overview of global processes that are responsible for global climate change, see chapters 2 and 3 of the first edition of Canada’s Changing Climate Report (CCCR2019). An overview of the spatial and temporal scales of the processes assessed in this chapter is in Figure 4.1.

Figure take-away: Atmosphere-ocean processes and phenomena that influence climate change in Canada occur on a wide range of time and space scales

Figure title: Atmosphere-ocean processes relevant to climate change in Canada and assessed in this chapter

Figure 4.1: Diagram of atmosphere-ocean processes relevant to climate change in Canada by spatial and temporal scale. The processes assessed in this chapter are the North Atlantic Oscillation (NAO), the Pacific–North American (PNA) pattern, the Atlantic Multidecadal Oscillation (AMO), the Pacific Decadal Oscillation (PDO), the Atlantic Meridional Overturning Circulation (AMOC), the El Niño–Southern Oscillation (ENSO), jet streams, Arctic amplification, extratropical storms, atmospheric blocks, hurricanes, atmospheric rivers, and large-scale thunderstorm conditions. A description of each process can be found in Box 4.1. The numbers in parentheses refer to the section of this chapter that assesses the process in question.
Long description

The figure is a schematic diagram showing major atmosphere–ocean processes that influence climate in Canada, arranged by the time and space scales on which they operate. The vertical axis spans seconds to centuries, and the horizontal axis spans 1 km to 10,000 km. Rectangular boxes denote individual processes and span the approximate time and space scales over which they act. Processes that operate on century‑long or multi-decadal timescales and basin‑scale distances include the Atlantic Meridional Overturning Circulation and Atlantic Multidecadal Oscillation, while Arctic amplification spans the entire Arctic. Processes such as the Pacific Decadal Oscillation and North Atlantic Oscillation span decadal to sub-seasonal timescales and continental‑to‑hemispheric spatial scales. El Niño–Southern Oscillation and Pacific–North American patterns act on interannual to seasonal scales. Jet streams, extratropical storms, atmospheric blocks, hurricanes, atmospheric rivers, and large‑scale thunderstorm environments occur on daily to weekly timescales and regional to continental distances.

At the smallest scales, thunderstorms occur over distances of a up to ten kilometres and on timescales of minutes to hours.

Overall, the diagram highlights that the atmosphere–ocean phenomena affecting Canada’s climate function across a wide range of spatial and temporal scales.

Regional variations in climate and climate change in Canada are partly governed by thermodynamic processes. Thermodynamic processes are those linked to changes in radiation and heat fluxes and have a direct connection to climate and climate change through their impacts on temperature and humidity. These processes often include feedbacks, where a particular change in the climate system drives a change in another aspect of the climate system that amplifies or weakens the original change. Feedbacks lead to a phenomenon known as Arctic amplification, that is, the Arctic region’s faster increase in surface temperature compared to the global average. This phenomenon largely explains why Canada is warming at a faster rate than the global average (see also FAQ 4.1), and why northern Canada is warming at a faster rate than southern Canada. Arctic amplification is assessed in section 4.2.

Regional variations in Canadian climate and climate change in Canada are also shaped by dynamical processes. These processes are responsible for the large-scale circulation of air and water. There is generally more uncertainty about human-induced changes in dynamical processes compared to thermodynamic processes (Shepherd, 2014). This is because changes in the large-scale circulation are usually the result of multiple, often competing processes. In addition, changes in the large-scale circulation often depend on changes in the spatial variations (or gradients) of large-scale thermodynamic conditions (such as those associated with Arctic amplification). The large-scale atmospheric circulation shapes regional variations in Canadian temperature and precipitation. For example, since the winds over mid-latitudes blow most often from west to east, relatively temperate and humid ocean air is transported to Canada’s west coast, making this region’s climate more temperate and humid than other parts of Canada. Also, the coldest days of the year are typically experienced when cold Arctic air is transported south by winds that blow from north to south. Changes in the strength and direction of winds will therefore lead to regional changes in surface temperature and precipitation.

A complicating factor in understanding past trends in the large-scale circulation is the fact that trends over periods shorter than a few decades are often dominated by internal climate variability, that is, fluctuations in the climate that are not caused by external climate forcings (Chapter 3, section 3.3.3). Since it is often not clear which part of the observed changes is due to external climate forcings (such as increasing greenhouse gases in the atmosphere due to human activity) and which part is due to internal climate variability, determining the cause of past trends can be challenging. Internal climate variability in Canada manifests itself on essentially all timescales and is the result of complex interactions in the climate system. It is often associated with “modes of internal variability,” meaning elements of the climate system that generally alternate between one set of patterns (or phase) and another (such as the El Niño–Southern Oscillation). These modes are often the result of feedbacks that lead to organized, large-scale fluctuations on timescales of weeks to decades. While this chapter focuses on trends in climate averaged over longer periods (typically 30 years), we also consider how modes of internal climate variability can be influenced by external climate forcing (such as greenhouse gas emissions due to human activity). Separating changes that are externally forced from those that are due to internal climate variability is particularly challenging when external climate forcing results in patterns of average change that resemble one of the phases of a mode of internal climate variability. Atmospheric modes of variability (such as the North Atlantic Oscillation) are discussed in section 4.3, and coupled atmosphere-ocean modes (including the El Niño–Southern Oscillation) are discussed in section 4.8.

Large internal climate variability also introduces uncertainty about projections of the atmospheric circulation and associated regional changes in temperature and precipitation. The projected near-term changes in low-level west-to-east wind, surface temperature, and precipitation simulated by version 5 of the Canadian Earth System Model are shown in Figure 4.2. An ensemble of 50 simulations was run with identical external climate forcings but with small perturbations through which different “realizations” of internal climate variability were generated (Chapter 3, section 3.3.3). The first column shows the average of the 50 simulations, in which the effect of internal climate variability is averaged out and hence represents the projected change caused by external climate forcings. Differences in responses between these simulations are unrelated to external climate forcings and are therefore the result of internal climate variability. The impact of this internal climate variability is illustrated by the second and third columns, which show projections in two simulations with opposing changes in wind. The simulation with a projected increase in wind over the Pacific Ocean (realization #13) features more transport of relatively warm and humid ocean air into western Canada, resulting in more warming and precipitation over western Canada than the simulation with a projected decrease in wind over the Pacific Ocean (realization #35). As internal climate variability cannot be predicted more than a few years in advance and these are projections for the near term relative to the pre-industrial period (approximated in this report as 1850 to 1900), both simulations are equally plausible. The large difference in regional climate responses between these two simulations highlights the large degree of uncertainty about regional climate change caused by internal climate variability, especially with regard to changes in precipitation.

Figure take-away: Internal climate variability has a large influence on the projections of the atmospheric circulation and associated temperature and precipitation patterns.

Figure title: Wind, surface temperature, and precipitation projections in a large ensemble of climate model simulations

Figure 4.2: Maps of future changes across western North America in winter west-to-east wind speed at 700 hPa (about 3 km above the surface), surface temperature, and precipitation as simulated by CanESM5. Projected changes are for the near term (2021–2040) and are relative to the pre-industrial period (1850–1900). The first column shows the average for a large ensemble of 50 simulations. The second and third columns show two individual simulations or “realizations” of internal climate variability. The projected wind changes are indicated by blue and red shading in the top row. The pre-industrial average west-to-east wind speeds, indicated by the grey contour levels in the top row, with levels of 3 m/s, are shown to indicate the mean jet stream position, as a reference for where the projected wind changes occur. Model simulations were driven by an intermediate emissions scenario (SSP2-4.5). Ensemble members were all run under the same external forcings but with slight perturbations to the initial weather state of each ensemble member to generate distinct realizations of internal climate variability.
Long description

This figure compares projected winter changes for 2021–2040 (relative to 1850–1900) across western North America from the CanESM5 50 member large ensemble under the SSP2 4.5 scenario. It is a 3×3 grid: the first column shows the ensemble mean, the second and third columns two individual realizations (#13 and #35) that differ only by tiny initial condition perturbations; rows show, from top to bottom, west to east wind speed at 700 hPa (~3 km), near surface air temperature, and precipitation. In the top row, a diverging scale depicts wind changes (blues = weaker, reds = stronger), with grey contours every 3 m/s indicating the pre industrial winds; the ensemble mean shows broad, forced patterns, whereas the single realizations exhibit strong regional departures, illustrating the impact of internal variability. The middle row shows temperature changes (reds = warming), with widespread warming that is largest toward the north. The bottom row shows precipitation changes (greens/teals = increases, tans/browns = decreases), revealing spatially varied wetting and drying that differs markedly between realizations even under identical external forcing. Overall, the figure demonstrates that internal climate variability can substantially reshape regional wind, temperature, and precipitation patterns around robust, ensemble mean signals.

An additional common challenge in assessing changes in large-scale phenomena is the fact that there is some subjectivity in how these phenomena are defined. For example, as discussed in section 4.4, there are several complementary definitions of atmospheric blocks commonly used in the scientific literature. Observed and projected trends can be sensitive to the definition, which introduces additional uncertainty. This also applies to atmospheric rivers, discussed in section 4.5.

The outline of this chapter is as follows. In section 4.2, we assess changes in Arctic amplification and their implications for Canadian temperatures. In sections 4.3 to 4.6, we assess changes in the horizontal large-scale atmospheric circulation that impact Canada’s average climate and climate extremes. Section 4.3 focuses on jet streams, storm tracks, and atmospheric modes of variability, such as the North Atlantic Oscillation. Section 4.4 focuses on changes in extratropical storms, extratropical high-pressure systems, and atmospheric blocks that affect Canada. Section 4.5 assesses changes in atmospheric rivers, while section 4.6 assesses changes in North Atlantic hurricanes. Changes in the vertical atmospheric circulation, and in particular changes in the large-scale environmental conditions that favour the development of thunderstorms over Canada, are assessed in section 4.7. Finally, sections 4.8 and 4.9 assess large-scale processes that involve the ocean. Changes in atmosphere-ocean coupled climate processes that impact the amplitude of year-to-year and decade-to-decade variability in Canadian climate, such as El Niño and La Niña, are assessed in section 4.8. Changes in the ocean circulation and its impact on Canadian climate are assessed in section 4.9.

Box 4.1 Terminology

Arctic amplification: Faster increase in temperature in the Arctic region compared to the global average

Atlantic Meridional Overturning Circulation (AMOC): Major ocean current system transporting heat to the North Atlantic, affecting climate variability in the North Atlantic and over adjacent land masses, including eastern Canada

Atlantic Multidecadal Oscillation (AMO): Climate pattern and mode of variability characterized by fluctuations in sea surface temperatures and air pressure in the Atlantic Ocean on decadal timescales, affecting decadal climate variability in eastern Canada

Atmospheric blocks: Strong high-pressure weather systems that move very slowly, often causing long periods of very cold or very warm conditions

Atmospheric rivers: Long, narrow and transient corridors of strong horizontal water vapour transport that are closely related to jet streams and extratropical storms

El Niño–Southern Oscillation (ENSO): Climate pattern and mode of variability characterized by fluctuations every two to seven years in sea surface temperatures and air pressure in the tropical Pacific Ocean, affecting year-to-year climate variability across much of the earth, including western and central Canada

Extratropical storms: Low-pressure weather systems occurring outside the tropics (also commonly known as extratropical cyclones)

Extratropical high-pressure systems: High-pressure weather systems occurring outside the tropics, accompanied by clear, sunny conditions (also commonly known as extratropical anticyclones)

Hurricanes: Very strong tropical cyclones forming in the Atlantic or eastern Pacific (see also “Tropical cyclones” below)

Jet streams: Strong bands of wind that typically flow from west to east throughout the lowest 15 km of the atmosphere, separating cold polar air from warm tropical air

Large-scale thunderstorm environment: Large-scale (in the order of 100 to 1000 km) atmospheric conditions that determine how easy or hard it is for thunderstorms to develop

North Atlantic Oscillation (NAO): Climate pattern and mode of variability characterized by fluctuations in atmospheric pressure in the North Atlantic affecting climate variability in that region, including eastern Canada, especially in winter

Pacific Decadal Oscillation (PDO): Climate pattern and mode of variability characterized by fluctuations in sea surface temperatures and air pressure in the Pacific Ocean on decadal timescales, affecting decadal climate variability in western and central Canada

Pacific–North American teleconnection pattern (PNA): Atmospheric pattern of variability modulated by the El Niño–Southern Oscillation (see above) that influences North American temperature and precipitation

Thunderstorms: Small-scale (in the order of kilometres) intense storms that are associated with strong upward air motion (also commonly known as convective storms)

  • Note: In scientific literature, “convective storms” often include other small-scale weather phenomena such as tornadoes, but for simplicity we use the term “thunderstorms” in this chapter. 

Tropical cyclones: Low-pressure weather systems that initiate over tropical oceans

  • Note: Very strong tropical cyclones in the Atlantic Ocean are also referred to as hurricanes, whereas other (weaker) tropical cyclones are also referred to as tropical storms.

Figure take-away: A visual snapshot of the contents of this chapter and of important cross-chapter linkages.

Figure title: Visual guide to the content of Chapter 4 and key cross-chapter linkages

Figure 4.3: Visual guide to Chapter 4 content and cross-chapter linkages.
Long description

Figure 4.3 is a conceptual diagram that serves as a roadmap for Chapter 4 and points readers to important cross-chapter connections. At the top, a box displays the chapter title and a short statement describing the chapter’s overall purpose. Below, other boxes list the chapter’s main sections, boxes, case stories, and frequently asked questions. Another box lists important cross-chapter connections to help readers find related information on topics covered in this chapter.

4.2: Arctic amplification

Key message 4.1: The Arctic (the region north of the Arctic circle) has warmed at more than three times the rate of the global average over the past five decades (high confidenceFootnote 2 ). Most of this increased warming, known as Arctic amplification, is caused by human influence (high confidence) and involves local climate processes and feedbacks, including sea ice loss. It largely explains why Canada has warmed nearly twice as fast as the global average and the Canadian Arctic three times as fast for the period 1970-2023 (high confidence).

Key message 4.2: Arctic amplification, and the greater rate of warming in Canada’s Arctic compared to the rest of Canada, will continue over the 21st century (very high confidence). In the coming decades, the Canadian Arctic is projected to warm at more than twice the rate of the global average (medium confidence).

4.2.1: Effects on Canadian weather and climate

As described in Chapter 2, in FAQ 4.1, and previously in CCCR2019, Canada and, to a greater extent, northern Canada are warming faster than the global average. This is largely related to a phenomenon known as Arctic amplification, the Arctic region’s faster increase in surface temperature compared to that of most other regions of the world (Holland & Bitz, 2003; Previdi et al., 2021; Serreze & Barry, 2011; Taylor et al., 2022). The rapid warming of the Arctic is having profound impacts on sensitive Arctic ecosystems and on First Nations, Inuit, and Métis livelihoods and ways of life (Hancock et al., 2022; Moon et al., 2024).

The Intergovernmental Panel on Climate Change (IPCC) Sixth Assessment Report (AR6) Working Group I (WGI) (IPCC AR6 WGI) determined (see section 7.4.4.1.3 in Forster et al., 2021) that there is high confidence that Arctic amplification “is a robust feature of the long-term response to greenhouse gas forcing.” Arctic amplification is quantified using the Arctic amplification factor, meaning the ratio of Arctic average surface temperature change to global average surface temperature change. Thus, a value greater than 1 indicates that the Arctic has warmed at a greater rate than the global average.

Arctic amplification is primarily driven by local climate feedbacks that act to amplify the warming from increasing atmospheric greenhouse gas concentrations. For example, Arctic warming leads to increased snow and sea ice melt, decreasing the amount of solar radiation that is reflected, which then further increases Arctic warming. These positive (amplifying) feedbacks are typically referred to as the snow and sea ice albedo feedbacks (see Box 4.2 for more information about the processes and feedbacks contributing to Arctic amplification). Arctic amplification affects the entire Arctic and thus impacts temperatures in northern Canada. Arctic amplification contributes to greater warming in Canada compared to the global average and greater observed warming in northern Canada compared to southern Canada, as well as to the seasonal patterns of warming in Canada, with a peak in late fall and early winter (Box 4.2, FAQ 4.1; Chapter 2, section 2.4.1). These spatial and seasonal patterns show up in the observed increase in surface temperature across the country (Chapter 2, section 2.4.1) and the observed decrease in the intensity and frequency of extreme cold spells, particularly in northern Canada (Chapter 8, section 8.2.1), and are related to a decline in snow cover and sea ice (Chapter 6, sections 6.2.2 and 6.3.2). Arctic amplification does not substantially change either the north-south meandering of the jet stream or storm tracks (section 4.3, Box 4.4).

Arctic amplification is causing significant environmental changes in northern Canada. Thawing permafrost and melting glaciers and sea ice (Chapter 6) can release stored contaminants like mercury into the Arctic environment. These changes pose serious risks to both wildlife and human health. Learn more about these impacts in Section 6.3.4 of the Northern Canada chapter of the Regional Perspectives Report, a report contributing to the Canada in a Changing Climate: National Assessment Process.

Box 4.2: Processes and feedbacks contributing to Arctic amplification

The response of the regional surface temperature to climate forcings, such as increasing greenhouse gas concentrations, depends on processes and feedbacks in the climate system. Thus, Arctic amplification can be understood by examining the relative contributions of these processes and feedbacks, and the contribution from the climate forcing itself, to Arctic warming and global or tropical warming. As shown in Box 4.2 Figure 1, these contributions to warming can be quantified using climate model simulations.

Figure take-away: Climate feedbacks amplify Arctic warming in response to increasing atmospheric CO2.

Figure title: The relative contributions of climate feedbacks to Arctic and tropical warming in response to increasing atmospheric CO2 concentrations

Box 4.2 Figure 1: Contributions to Arctic (60–90°N) and tropical (30°S–30°N) surface temperature change at year 100 following an abrupt quadrupling of atmospheric carbon dioxide (CO2) in simulations with CMIP5 climate models. The feedback contributions shown are for the lapse rate (LR), snow and sea ice albedo (A), water vapour (WV), and cloud (C) feedbacks, and the latitudinal variation in the Planck feedback (P’, the local difference from its global average value). The additional contributions shown are for the latitudinal variation of the climate forcing associated with CO2, atmospheric heat transport convergence (ΔAHT), and ocean heat uptake (ΔOHU). The feedbacks are expressed as contributions to the surface temperature change and sum to the total simulated temperature change for the Arctic and the tropics. Source: Figure 3 in Goosse et al. (2018).
Long description

This graph shows Arctic warming on the vertical axis and tropical warming on the horizontal axis. A diagonal line from lower left to upper right separates the graph into upper and lower halves. The warming contributions of eight climate feedbacks and other processes are shown by coloured dots. The extent to which these feedbacks and other processes contribute to Arctic amplification can be determined by the perpendicular distance of the corresponding dot from the diagonal line. Dots in the upper half of the graph indicate those feedbacks or processes that contribute to enhanced warming in the Arctic relative to the Tropics: lapse-rate, albedo and Planck feedbacks and atmospheric heat transport. Dots in the lower half indicate those that contribute to enhanced warming in the Tropics relative to the Arctic: water vapour and cloud feedbacks, ocean heat transport and the climate forcing associated with carbon dioxide. Together the dots in the upper half of the graph are a greater perpendicular distance from the diagonal line and, thus, these feedbacks and processes lead to enhanced warming in the Arctic relative to the tropics.

In Box 4.2 Figure 1, the extent to which particular feedbacks, forcings, or other processes contribute to Arctic amplification can be determined by the perpendicular distance of the corresponding point from the 1:1 line. Points that fall along the 1:1 line indicate that a feedback, forcing, or process contributes equally to Arctic and tropical surface temperature change and therefore does not contribute to Arctic amplification. The following feedbacks and other processes can intensify or lessen Arctic amplification:

  • Planck feedback: The Planck feedback causes the Earth’s surface to warm in order to restore energy balance in response to greenhouse gas forcing; the warming required to restore energy balance is greater in cold regions like the Arctic, which contributes to Arctic amplification.
  • Lapse rate feedback: The lapse rate is the rate at which the atmospheric temperature falls with altitude. Changes in the lapse rate as the surface warms can affect the vertical fluxes of energy. In the tropics, increasing greenhouse gases tend to warm the upper troposphere more than the surface, decreasing the lapse rate. This makes the atmosphere radiate more effectively to space, partially decreasing the effects of the increasing greenhouse gases, which is a negative feedback. The opposite occurs in the Arctic where warming tends to be largest near the surface and the lapse rate feedback is positive, which contributes to Arctic amplification.
  • Snow and sea ice albedo feedbacks: Snow and sea ice reflect solar radiation. As the surface warms, snow and sea ice melt, exposing darker surfaces that absorb more solar radiation, leading to greater warming and contributing to Arctic amplification.
  • Water vapour feedback: The water vapour feedback is associated with the atmosphere’s capacity to hold more water vapour as it warms, and is a strong positive feedback because water vapour itself is a greenhouse gas. In the Arctic, where the atmosphere is relatively dry, this feedback is weaker than in the tropics and thus opposes Arctic amplification.
  • Atmospheric heat transport: Transport of heat into the Arctic contributes to Arctic amplification. However, the contribution of this transport to Arctic amplification is uncertain due to compensation between an increase in moisture transport and a decrease in dry static energy transport and large internal climate variability (Hahn et al., 2021).
  • Cloud feedbacks and ocean heat uptake: Cloud feedbacks, feedbacks associated with changes in cloud properties as the climate warms, and ocean heat uptake weakly oppose Arctic amplification (Hahn et al., 2021).

The primary positive (amplifying) feedbacks contributing to Arctic amplification are the temperature feedbacks (lapse rate and Planck) (Pithan & Mauritsen, 2014) and the snow and sea ice albedo feedbacks (Dai et al., 2019; Screen & Simmonds, 2010). Both the positive snow and sea ice feedbacks, and the lapse rate feedback (which is positive in the Arctic), are directly connected to the loss of Arctic sea ice due to global warming (Dai et al., 2019; Feldl et al., 2020). With increasing snow and sea ice melt in summer and fall due to global warming, more energy is absorbed in the ocean surface. As fall turns to winter and the air temperature becomes colder than the ocean temperature, the additional energy in the ocean is exchanged with the atmosphere. The resulting near-surface warming increases the lapse rate, which further amplifies the warming through the lapse rate feedback. The seasonality of these two feedbacks leads to a distinct seasonality of Arctic amplification, with a peak in late fall (Dai et al., 2019; Feldl et al., 2020; Pithan & Mauritsen, 2013).

Uncertainty about the magnitude of the relative contributions of all the above processes and feedbacks to Arctic amplification is due to differences across models (Hahn et al., 2021; Pithan & Mauritsen, 2014), sensitivities of the feedbacks to the amount of warming (Dai et al., 2019; Holland & Landrum, 2021; S.-N. Zhou et al., 2023), the type of climate forcing (e.g., CO2 versus non-CO2 climate forcings) (Liang, Polvani, Previdi, et al., 2022; Polvani et al., 2020; Sigmond et al., 2023; Stjern et al., 2019), the method used to diagnose the feedbacks (Hahn et al., 2021; Janoski et al., 2024), and internal climate variability (Hahn et al., 2021).

4.2.2: Past changes and their causes

Surface temperature measurements in the Arctic consist of land-based weather station measurements of surface air temperature and sea surface temperature measurements from buoys and ships. However, because of the perennial ice cover across much of the Arctic Ocean, measurements in the central Arctic are limited. Global gridded observational data products (see Figure 4.4 and FAQ 4.1 Figure 1 for examples and Chapter 2, section 2.3.3, for a detailed description) therefore employ interpolation techniques (estimations of unknown data based on known data) to fill in the gaps in data-sparse regions like the Arctic contributing to uncertainty about Arctic surface temperature trends  (see section 2.3.1.1.3 in Gulev et al., 2021; Lenssen, 2022). When in-situ (on-location) data, satellite data, or reanalysis data (explained below) are used to assess these interpolated data products, interpolation is found to improve estimates of global and Arctic averaged temperature change compared to the alternative of estimates that ignore regions with little or no data (Cowtan & Way, 2014; Lenssen et al., 2019; Simmons et al., 2017). Although gridded observational data products have improved, there has been a recent reduction in in-situ data gathering in the Arctic due to both the decline in the number of weather stations across Canada’s North (Voosen, 2023) and the exclusion of Russia from internationally coordinated Arctic monitoring programs since 2022 (López-Blanco et al., 2024; Witze, 2022). This reduction may introduce a bias in regional estimates of Arctic surface temperature. Reanalysis data products provide a complementary but not independent alternative to gridded observational data products (Chapter 2, section 2.3.3). Reanalysis data products are numerical representations of the recent past global climate and are produced by combining a collection of in-situ and satellite observations of the atmosphere, land surface, and ocean with state-of-the-art weather forecast models. They provide temporal and spatial consistency and completeness. In the remainder of section 4.2.2, both gridded observational data products and reanalysis data will be assessed.

Figure take-away: Arctic warming and Arctic amplification have become stronger in recent decades.

Figure title: Past surface temperature trends and local amplification for the Arctic and sub-Arctic regions

Figure 4.4: Maps of annual average surface temperature trends and the local amplification factor (the local surface temperature trend divided by the global average surface temperature trend) calculated for the periods 1950–2023 and 1970–2023, derived from the average of four observational datasets. In a) and c), the dots indicate where the local trends are statistically significant at the 5% level (meaning there is a ≤ 5% chance of concluding that an effect or trend exists when it does not). In b) and d), values greater than 1 indicate more local warming than the global average, values between 0 and 1 indicate less local warming than the global average, and values less than 0 indicate local cooling. The dashed line in b) and d) depicts the Arctic Circle (66.5oN latitude). The data consist of the average of four surface temperature data products. Data source: three observationally based gridded products, GISTEMP (Lenssen et al., 2019), HadCRUT5 (Morice et al., 2021), and Berkeley Earth (Rohde & Hausfather, 2020), and one reanalysis product, ERA5 (Hersbach et al., 2020).
Long description

The figure contains four maps arranged in two rows and two columns. The maps are centred on the North Pole and extend southward to a latitude of 50°N. The maps show coloured shading indicating annual average surface temperature trends in the left column and local amplification factors in the right column for two time periods: 1950–2023 in the top row and 1970–2023 in the bottom row.

Coloured shading for surface temperature trends (left column) indicates warming across Canada (red shades), with greater warming towards the North pole and greater warming in the 1970-2023 time period. Black dots are overlaid on the shading and cover the entire map except for a region in the North Atlantic. The dots indicate locations where the trend is statistically significant.

Coloured shading for the local amplification factor (right column) indicates amplification (values greater than 1) across Canada (red shades), with greater amplification towards the North pole and greater amplification in the 1970-2023. A dashed circular line marks the Arctic Circle at 66.5°N in each panel in the right column, highlighting regions of stronger amplification.

Since the mid-20th century, the Arctic has been warming at a faster rate than the global average (Figure 4.4). Given this updated analysis and previous studies, there is high confidence that annual average surface temperature in the Arctic as a whole has warmed at more than three times the rate of the global average since the 1970s (Figure 4.4d) (Chylek et al., 2022; Douville, 2023; Lenssen, 2022; Rantanen et al., 2022). This is equivalent to an Arctic amplification factor of more than 3. Arctic amplification peaks in late fall and reaches a low in summer (Box 4.1) (Previdi et al., 2021; Rantanen et al., 2022; Taylor et al., 2022), and the region with the greatest amplification corresponds to the region with the greatest sea ice loss (Previdi et al., 2021). Arctic amplification has contributed to past warming rates of close to two times in Canada and three times in the Canadian Arctic compared to the global average (FAQ 4.1). Studies estimate that Arctic amplification only became discernable during the late 20th century (England et al., 2021). Before then, Arctic warming from anthropogenic (human-caused) greenhouse gas emissions was masked by large internal climate variability and the cooling effect of anthropogenic aerosols, that is, particulates in the air created by human activities such as burning fossil fuels (X. Chen & Dai, 2024; Douville, 2023; England et al., 2021; Holland & Landrum, 2021; Najafi et al., 2015; Previdi et al., 2023; Y.-T. Wu et al., 2024).

There is high confidence that most of the observed Arctic amplification is due to human activities. Three independent studies calculated the human-caused part of Arctic amplification by removing from the observations for 1979 to 2022 the part of Arctic amplification that is due to internal climate variability. They found that human activity is responsible for 75% of the observed Arctic amplification. The Arctic amplification factor associated with human activity is close to the corresponding value in the multi-model average (Douville, 2023; Sweeney et al., 2023; W. Zhou et al., 2024).

4.2.3: Future changes

Arctic amplification will continue to be a dominant pattern of climate change over the 21st century (very high confidence) (Davy & Griewank, 2023; Douville, 2023; see Section 7.4.4.1.3 in Forster et al., 2021; Ono et al., 2022; Y. Wu et al., 2023). This is consistent with projected warming for Canada, where Arctic amplification will continue to contribute to greater warming in northern Canada compared to southern Canada (Chapter 3). There is medium confidence in the projected magnitude of Arctic amplification, however, with Arctic warming by the end of the century ranging from 1.5 to 3.5 times the global average across climate models (Hay et al., 2024; Linke et al., 2023; Ono et al., 2022). Because Arctic amplification reflects the warming of the Arctic relative to the global average (the ratio of Arctic warming to global warming), it is relatively insensitive to the emissions scenario (Hay et al., 2024). The large range in projected Arctic amplification primarily results from internal climate variability and differences in the representation of climate feedbacks between models, which can affect the projected rate of both global and Arctic warming (Z. Cai et al., 2021; Y. Wu et al., 2023).

While Arctic amplification will continue over the 21st century, climate models project a shift in the timing of peak Arctic amplification from late fall to early winter as the sea ice minimum occurs later in the fall, particularly for high emissions scenarios (medium confidence). The projected time frame for this shift from fall to winter is uncertain, reflecting both model differences and internal climate variability (Davy & Griewank, 2023; Douville, 2023; Hahn et al., 2022; Holland & Landrum, 2021; Liang, Polvani, & Mitevski, 2022; Taylor et al., 2022; Y. Wu et al., 2023).

In addition to a projected shift in the seasonal timing of Arctic amplification, some studies suggest that the annual average strength of Arctic amplification peaks and then declines with additional warming. As the climate warms, there is less snow and sea ice available to melt. This reduces the amplifying snow and sea ice albedo feedbacks. As a result, subsequent warming will be less amplified in the Arctic, which contributes to a decline in the magnitude of the Arctic amplification factor (see Box 4.1 for more information on climate feedbacks) (Dai et al., 2019; Davy & Griewank, 2023; Douville, 2023; Holland & Landrum, 2021). A decline in Arctic amplification may also result from a decrease in poleward heat transport by the Atlantic Meridional Overturning Circulation (section 4.9) (W. Liu et al., 2020). There is substantial uncertainty about the projected year and strength of a peak-and-decline due to the large amount of variability across models (Davy & Griewank, 2023; Douville, 2023). Additional uncertainty about a projected peak-and-decline is due to a sensitivity to the reference period: a peak-and-decline of Arctic amplification is projected when using mid-to-late 20th-century reference periods, but not when using a pre-industrial reference period (Hay et al., 2024). Overall, confidence in a projected peak-and-decline in Arctic amplification is low. It is important to note that a future decline in the magnitude of Arctic amplification would not indicate that the Arctic is no longer warming, but that the rate of Arctic warming relative to global warming is declining.

Projected trends for the Canadian Arctic are similar to what is described above for the entire Arctic. CMIP6 models project that the Canadian Arctic amplification factor will stabilize around an annual average value of slightly more than 2 (medium confidence; Figure 4.5a). This is consistent with what is observed, given the large role of internal climate variability in the observational record (section 4.2.2). Models also project a shift in seasonal timing of Arctic amplification in the Canadian Arctic (Figure 4.5b), which is most pronounced in high (SSP3-7.0) and very high (SSP5-8.5) emissions scenarios for the Canadian Arctic.

Figure take-away: Arctic amplification in Canada stabilizes in the near term and the seasonal timing shifts from late fall to early winter by late-century.

Figure title: Projected evolution of Arctic amplification in Canada with warming

Figure 4.5: The multi-model average Arctic amplification factor averaged over the Canadian Arctic for 21 CMIP6 climate models. a) Annual average Arctic amplification factor as a function of year. b) Seasonal cycle of the Arctic amplification factor averaged for the near term (2021–2040) and the late century (2081–2100). The numerator (the Arctic warming) and the denominator (the global warming) of the Arctic amplification factor for each model are computed as the differences between the average of a running 30-year period and the average of the reference period of 1850 to 1900. The x-axis of a) represents the last year of each 30-year period. Climate model output includes historical simulations for before 2015 and projections for 2015 and onwards based on the intermediate emissions scenario (SSP2-4.5). Dark and light grey shading in a) show the 95% confidence interval (CI) and full range across the 21 models, respectively. The vertical dashed lines in b) indicate the month with the highest Arctic amplification factor, and the light blue and pink shading show the 95% confidence intervals across the 21 models. The Canadian Arctic is bounded by 66.5°N to 83.11°N and 219°E to 307.38°E.
Long description

The figure contains two panels illustrating the Arctic amplification factor for the Canadian Arctic. The left panel presents a time series of annual, multi model average amplification, shown as a solid black curve. The horizontal axis spans years from 1995 to 2100, while the vertical axis ranges from 0.75 to 3.25. The amplification factor increases rapidly from roughly 1.5 to about 1.8 between 1995 and 2010, followed by a more gradual rise toward a value near 2 by 2100. Dark grey shading around the line represents the 95% confidence interval across the climate models, and lighter grey shading depicts the full spread of model results.

The right panel shows the seasonal cycle of the amplification factor for two future periods. The horizontal axis lists months from June to May, and the vertical axis again ranges from 0.75 to 3.25. Two coloured curves display the multi model averages: blue for the near term period (2021–2040) and red for the late century period (2081–2100). Light blue and pink shading indicate the corresponding 95% confidence intervals. The curves are somewhat bell-shaped, with minima in the summer months and maxima in the late fall and early winter. A vertical dashed line marks the month of maximum amplification for each period, which shifts from November in the near term to December by late century.

4.2.4: Confidence terms in key messages: summary of evidence

Key message 4.1: The Arctic (the region north of the Arctic circle) has warmed at more than three times the rate of the global average over the past five decades (high confidence). Most of this increased warming, known as Arctic amplification, is caused by human influence (high confidence) and involves local climate processes and feedbacks, including sea ice loss. It largely explains why Canada has warmed nearly twice as fast as the global average and the Canadian Arctic three times as fast for the period 1970-2023 (high confidence).

Key message 4.2: Arctic amplification, and the greater rate of warming in Canada’s Arctic compared to the rest of Canada, will continue over the 21st century (very high confidence). In the coming decades, the Canadian Arctic is projected to warm at more than twice the rate of the global average (medium confidence).

In summary, we have high confidence that the Arctic has warmed more than three times faster than the global average, and that this is contributing to the nearly two times greater observed warming in Canada and three times greater observed warming in the Canadian Arctic in recent decades. Moreover, we have high confidence that most of the recent Arctic amplification is attributable to human-caused climate change. This assessment is supported by evidence from multiple studies and analyses based on various observational and reanalysis data products, historical climate model simulations, and theoretical understanding of Arctic amplification, and is consistent with the IPCC AR6 WGI assessment.

We have very high confidence that Arctic amplification will continue over the 21st century and will continue to contribute to greater warming in the Canadian Arctic compared to southern Canada. This assessment is based on multiple studies and analyses using CMIP6 climate model projections and is consistent with the IPCC AR6 WGI assessment. Our medium confidence in the future strength of Canadian Arctic amplification, with an annual average value of slightly more than 2, is due to large internal climate variability, and climate model uncertainty about the relative contributions of the numerous climate feedbacks that cause Arctic amplification.

4.3: Jet streams, storm tracks, and atmospheric modes of variability

Key message 4.3: Changes in recent decades in the jet streams and storm tracks that affect Canada are small and seen only in limited seasons and regions. There is low confidence in any human influence on these past changes. An overall poleward shift in the jet streams and storm tracks is projected by the end of the 21st century, but the changes are small and depend on the region and season (low confidence).

4.3.1: Effects on Canadian weather and climate

Jet streams are strong bands of wind that flow from west to east throughout the lowest 15 km of the atmosphere that are driven by temperature differences between high and low latitudes, and the Earth’s rotation (Figure 4.6). In the Northern Hemisphere, the strongest jet streams occur over the Pacific and Atlantic oceans. Jet streams are closely linked with extratropical storms (section 4.4), which travel from west to east and tend to occur just to the north of the jet stream in regions referred to as storm track regions. The position and strength of the jet streams vary naturally on all timescales from days to multiple decades. Changes in the position and strength of the jet streams are closely connected to modes of variability, like the North Atlantic Oscillation (NAO) and Arctic Oscillation (AO) (see Box 2.5 of CCCR2019). A positive phase of the AO is defined by lower than average pressure over the Arctic and higher than average pressure in the mid-latitudes, and is linked with a stronger, more poleward jet stream. The NAO is the regional manifestation of the AO over the Atlantic, and its positive phase is associated with a stronger and more northward jet stream over the North Atlantic (Figure 4.7). The negative phases of the AO and NAO have opposite changes in pressure and the jet stream relative to the positive phases.

Variability in the jet streams can have a large influence on weather and climate variability in Canada, but the exact influence can vary by region and season. For example, a stronger jet stream in the North Pacific during winter causes warmer and wetter weather on the west coast. A stronger North Pacific jet stream is also associated with a strengthening of the storm tracks. This means stronger or more frequent extratropical storms or both affecting the west coast. Shifts in the position of the Pacific jet stream and associated storm tracks strongly influence the amount and location of precipitation on the west coast. A stronger and more poleward Atlantic jet stream (associated with the positive phase of the NAO) during winter brings colder temperatures and less precipitation on the east coast of Canada (Figure 4.7). During summer, extratropical storms bring cooler ocean air over land. As a result, weaker than normal storm tracks (weaker or fewer storms or both) tend to lead to warmer temperatures and extreme heat (Coumou et al., 2015). Because the jet stream separates colder air to the north from warmer air to the south (Figure 4.6), large meanders or waves in the jet stream are linked to extreme temperatures (Screen & Simmonds, 2014). For example, extreme events such as the Pacific Northwest heatwave of June 2021 (Neal et al., 2022) and the extreme cold across central and eastern Canada during the winter of December 2013 to February 2014 (Watson et al., 2016) were associated with large meanders in the jet stream.

Figure take-away: The position and strength of the jet streams affect regional weather and climate.

Figure title: Illustration of the jet stream, and associated temperature anomalies

Figure 4.6: Illustration of the jet stream. Jet streams are strong bands of wind that flow from west to east, with bends to the north and south, often referred to as meanders. These meanders separate relatively cold air to the north (blue shading) and warm air to the south (orange shading). The location and magnitude of the meanders vary from day to day. Credit: NOAA/JPL-Caltech.
Long description

This is an Illustration of the jet stream over a map of North America. Jet streams are strong bands of wind that flow from west to east, with bends to the north and south, often referred to as meanders. These meanders separate relatively cold air to the north and warm air to the south. The location and magnitude of the meanders vary from day to day. In this illustrative image, there is a deep southern meander in the jet stream that allows cold air from the north to extend down into southern Canada over the Great Lakes region. Credit: NOAA/JPL-Caltech

Unlike changes directly associated with temperature, it is not clear from physical reasoning how jet streams, storms tracks, and modes of variability might change in a warming climate. This uncertainty is due to the opposing influences of various processes that all have uncertain magnitudes (T. Shaw et al., 2016). For example, strong warming in the Arctic due to Arctic amplification decreases the north-south temperature gradients in the lower troposphere of the Northern Hemisphere (section 4.2). This decrease in the lower troposphere opposes the increase in the north-south temperature gradient in the upper troposphere (around 10 to 15 km above the Earth’s surface) associated with increased warming in the tropics (see also Box 4.4) (Barnes & Polvani, 2015). Other processes, such as changes in clouds (Ceppi & Hartmann, 2015) and the strength of the circulation in the stratosphere (15 to 50 km above the Earth’s surface) (Karpechko et al., 2022), will also likely play a role in determining how jet streams may change in a warming climate.

Figure take-away: Each North Atlantic Oscillation phase is associated with a different winter climate pattern in Canada.

Figure title: The effects of the North Atlantic Oscillation on winter climate in Canada

Figure 4.7: Diagram of changes in prevailing climate conditions associated with the positive and negative phases of the North Atlantic Oscillation (NAO) during winter. See Supplementary Figure S4.1 for a more quantitative picture of the NAO impacts.
Long description

This schematic illustrates how the North Atlantic Oscillation (NAO) affects winter climate patterns across Canada by comparing its positive and negative phases. In the positive NAO, the pressure difference between the subtropical high and subpolar low is stronger, producing a strong jet stream that arcs from eastern North America toward Europe. Labelled ovals mark strong low pressure systems near Iceland and strong high pressure systems farther south. Over eastern and central Canada, broad blue shading indicates colder and drier winter conditions, while red shading over the southeastern United States and parts of the west indicates warmer conditions.

In the negative NAO, the pressure contrast weakens, leading to a weaker jet. Labelled ovals mark a weaker low pressure system near Iceland and stronger high pressure systems farther south. This is associated with warmer and wetter conditions over much of eastern and central Canada (shown in red), while blue shading to the southwest indicates colder temperatures. Together, the panels show how NAO phase changes influence winter temperature, precipitation, and storm track patterns across Canada.

4.3.2: Past changes and their causes

Past changes in the position and strength of jet streams are generally small relative to internal climate variability, are regionally complex, and can depend on the time period considered (Blackport & Fyfe, 2022; Manney & Hegglin, 2018; Simmons, 2022). The IPCC AR6 assesses that the jet streams “have likely been shifting poleward in both hemispheres since the 1980s with marked seasonality in trends (medium confidence)” (see section 2.3.1.4.3 in Gulev et al., 2021). In the Northern Hemisphere, the poleward shift is most evident over the Pacific Ocean during winter, where the trends since 1980 do not depend on the choice of dataset or how the position of the jet stream is defined (Keel et al., 2024).

One way to determine changes in the jet streams is by looking at changes in the west-to-east low-level winds (at about 3 km above the Earth’s surface). The poleward shift in the Pacific jet stream is indicated by stronger low-level west-to-east winds north of the average position of the jet stream and weaker low-level west-to-east winds south of the average position of the jet stream (Figure 4.8). The Pacific jet stream has generally shifted toward the North Pole in other seasons too, but the trends are weak and not statistically significant (Keel et al., 2024). Over the Atlantic Ocean, since 1980, the jet stream has strengthened in winter and spring, shifted toward the pole in fall, and shifted toward the equator in summer (Figure 4.8). The past trends can depend strongly on the start year they are calculated from. For example, when the trends are calculated starting from the mid-20th century instead of 1980, the trend toward a stronger winter North Atlantic jet stream is larger (Blackport & Fyfe, 2022) and the poleward shift in the winter Pacific jet stream is substantially weaker (Patterson & O’Reilly, 2025).

Attributing past trends to specific causes is challenging because of small signal-to-noise ratios in most regions and seasons. In addition, climate models perform poorly in reproducing past trends and variability (Blackport & Fyfe, 2022; Bracegirdle et al., 2018; Patterson & O’Reilly, 2025), making it difficult to understand the causes of the changes. Overall, confidence in attributing jet stream trends to human influence is low.

Figure take-away: The past trends in the strength and position of the Northern Hemisphere jet streams are generally weak and depend on the region and season.

Figure title: Past trends in low-level west-to-east wind speeds across Canada and surrounding oceans

Figure 4.8: Map of trends for 1979 to 2023 in west-to-east wind speed across North America at 700 hPa (about 3 km above the Earth’s surface) in a) winter (December-January-February), b) spring (March-April-May), c) summer (June-July-August), and d) fall (September-October-November). Wind speeds at this altitude in the atmosphere are an indicator of the strength of the jet stream. The grey contour lines indicate the average wind speeds of 6, 12 and 18 m/s for 1979 to 2023. The dots indicate where the trends are statistically significant after controlling for the false discovery rate at the 10% significance level (meaning there is a ≤ 10% chance of concluding that an effect or trend exists when it does not). Data source: ERA5 reanalysis.
Long description

This figure shows how west to east wind speeds at about 3 km above the surface (700 hPa) have changed across North America from 1979 to 2023, separately for winter, spring, summer, and fall. Each seasonal panel uses colour shading to indicate the wind speed change per decade, based on the ERA5 atmospheric reanalysis, with grey contours every 6 m/s indicating the 1979-2023 mean wind speeds. Blue areas show regions where the westerlies have weakened, while yellow to red areas indicate where they have strengthened. Black dots mark locations where the trends are statistically significant, meaning there is a low likelihood that the observed change occurred by chance. In winter, a pronounced band of decreased westerly flow appears over the Pacific, while spring shows more localized strengthening near the northwest Atlantic. Summer and fall display weaker, more spatially patchy changes overall. These seasonal patterns reveal how large scale atmospheric circulation has shifted over recent decades.

Changes in storm tracks are consistent with changes in jet streams. In winter, the Pacific storm track has strengthened (which is associated with stronger or more frequent extratropical storms or both) and shifted poleward (E. K. M. Chang & Yau, 2016). The Atlantic storm track has strengthened with little change in position since the mid-20th century, but over the shorter period since 1980 the strengthening has been small and not statistically significant (E. K. M. Chang & Yau, 2016). The causes of these changes are difficult to assess because of the small signal-to-noise ratios and lack of studies directly comparing historical model simulations and observations. However, the strengthening of the North Atlantic storm track and the poleward shift in the Pacific storm track are consistent with projections, but the strengthening of the Pacific storm track is not seen in projections (section 4.3.3). In summer, storm tracks have weakened (which is associated with weaker or fewer extratropical storms or both) over the Northern Hemisphere (Coumou et al., 2015), and this weakening is more pronounced over North America (E. K. M. Chang et al., 2016). The weakened summer storm tracks are also seen in historical climate model simulations (E. K. M. Chang et al., 2016; Chemke & Coumou, 2024; Kang et al., 2023) and can be attributed to human-caused forcing (medium confidence) (Chemke & Coumou, 2024; Kang et al., 2024). However, the mechanisms are not well understood (Kang et al., 2023).

Past trends in the NAO and AO are dominated by a large amount of variability over many decades, making it difficult to identify robust changes. Since the mid-20th century, there has been a trend toward the positive phase of the NAO and AO during winter (Blackport & Fyfe, 2022; Eyring et al., 2021a). The upward trend is primarily a result of a strong increase that occurred from the 1960s to the 1990s. This increase was followed by a reversal of the trend toward the negative phase of the NAO and AO from the 1990s until the early 2010s, and a period of a positive NAO and AO in the last decade. This has resulted in very weak trends since 1980, as also reflected in the weak trends in the winter Atlantic jet stream shown in Figure 4.8a. The observed upward trend in the winter NAO and AO since the middle of the 20th century is outside of the range of trends in model simulations, which indicate only a very weak upward trend on average (Blackport & Fyfe, 2022; Eyring et al., 2021b). The discrepancy between models and observations makes it challenging to understand and attribute the trends. There is evidence that the NAO showed a strong downward trend during summers from the 1990s until the early 2010s (Hanna et al., 2015). However, this trend has not continued, and the longer-term trends remain small relative to internal climate variability (Hanna et al., 2022).

Some studies have suggested that Arctic amplification (section 4.2, boxes 4.3, 4.4) has caused jet streams to become “wavier” over recent decades, meaning they have larger meanders (Cohen et al., 2020; Francis & Vavrus, 2012). However, the metrics used to measure jet stream waviness have been shown to be flawed, and better metrics show a lack of statistically significant trends (Barnes, 2013; Screen & Simmonds, 2013). Updated trends and metrics show little change in jet stream waviness since 1979 relative to internal climate variability over both the Northern Hemisphere and Canada (Blackport & Screen, 2020), despite substantial Arctic amplification.

Box 4.3: The polar vortex, the jet stream, and the impact of climate change

The polar vortex is a band of strong west-to-east winds encircling each of the Earth’s poles in the stratosphere, the atmospheric layer 15 to 50 km above the Earth’s surface. For the purposes of this box, the polar vortex refers to the Arctic polar vortex. It forms every fall when sunlight decreases near the pole, cooling the pole and increasing the equator-to-pole temperature difference, which drives these winds. The polar vortex breaks up every spring when sunlight returns to the pole. On average once every two winters, the polar vortex suddenly warms up and breaks down, an event known as a sudden stratospheric warming (Butler et al., 2015). In the weeks after a sudden stratospheric warming, the weather patterns in the troposphere (the atmospheric layer between the Earth’s surface and 15 km above the surface) often resemble the negative phase of the North Atlantic Oscillation (Figure 4.7), which leads to warmer than normal conditions in eastern Canada (e.g., Butler et al., 2017). There is a lot of variability in the polar vortex, and there is no evidence that it has changed in response to human-caused climate change (Seviour, 2017). Projected changes in the polar vortex are highly uncertain due to considerable year-to-year variability and model disagreement (Karpechko et al., 2022).

The polar vortex is often confused with the jet stream, a band of strong year-round west-to-east winds in the troposphere. The jet stream does not always blow in a straight path, since it can bend north and south in what we call a “wavy” jet stream. When it is wavy, cold air can move farther south, leading to cold snaps. It has been speculated that climate change is acting to slow down the jet stream, and that such a slowdown is making the jet stream wavier, potentially leading to more cold snaps. However, there is no robust evidence that jet stream waviness has increased over recent decades, and climate model simulations do not support this hypothesis. In addition, global warming has actually made cold extremes less frequent and less cold (Box 4.4; Chapter 8, section 8.2.1).

Box 4.4: Weak influence of Arctic warming on mid-latitude weather and climate

Much attention has been paid to the possibility that Arctic warming has and will influence mid-latitude weather and climate in the Northern Hemisphere. The proposed mechanisms are varied, but most reflect potential changes in the atmospheric circulation and extreme weather events associated with a reduction in the lower tropospheric pole-to-equator temperature gradient due to Arctic amplification (Barnes & Screen, 2015). The IPCC AR6 WGI report concluded that “there is low confidence in the relative contribution of Arctic warming to mid-latitude atmospheric changes compared to other drivers,” and that contrasting lines of evidence remain to be reconciled (Doblas-Reyes et al., 2021, Section 10.1.5, Cross-Chapter Box 10.1). The following summarizes and updates what was reported in the IPCC assessment report.

Evidence of an influence of Arctic warming on mid-latitude circulation from observational studies is inconsistent and weak for various reasons, namely, large internal climate variability (Blackport & Screen, 2020; Siew et al., 2020; Smith et al., 2022; J. L. Warner et al., 2020), differences in the choice of metric (e.g., Barnes, 2013; Francis & Vavrus, 2012; Screen & Simmonds, 2013), and difficulty disentangling cause and effect (e.g., Blackport et al., 2019).

Initial attempts to isolate the influence of Arctic warming on mid-latitude atmospheric circulation, using climate model experiments with prescribed Arctic sea ice loss, showed inconsistency across models and experimental designs (Screen et al., 2018). More recent coordinated model experiments, including the Polar Amplification Model Intercomparison Project (Smith et al., 2019), show that in isolation, sea ice loss tends to move the tropospheric jet toward the equator, but that the magnitude of this shift varies across models (Liang et al., 2024; Smith et al., 2022) and depends on systematic model biases (Sigmond & Sun, 2024; Smith et al., 2017). As noted in section 4.3, the location of the tropospheric jet is also affected by increased upper-level warming in the tropics, which tends to push the jet toward the pole. The opposing effect of Arctic amplification and upper-level tropical warming has been described as a “tug-of-war” on the jet stream, contributing to weak trends overall (Fraser-Leach et al., 2023; Hay et al., 2022; T. A. Shaw & Smith, 2022).

In addition to affecting the location of the tropospheric jet, some studies have suggested that Arctic amplification has increased the extent to which the jet meanders from north to south, possibly increasing the occurrence of winter cold extremes in the mid-latitudes. However, there is no robust evidence that the extent to which the jet meanders from north to south has changed or will change in response to global warming (section 4.3). In fact, there is both observational and climate model evidence of a decrease in the frequency and severity of cold extremes over North America, including Canada, due to southward transport of increasingly warmer Arctic air (Chapter 8, section 8.2.1), (Blackport et al., 2024; Blackport & Fyfe, 2024; Lo et al., 2023; Van Oldenborgh et al., 2019). As illustrated in Box 4.4 Figure 1, Polar Amplification Model Intercomparison Project experiments demonstrate that Arctic warming associated with sea ice loss leads to a decrease in the severity of cold extremes (Blackport & Fyfe, 2024; Lo et al., 2023).

Figure take-away: Arctic sea ice loss makes cold extremes across Canada less cold.

Figure title: Warming of cold extremes across Canada in climate model simulations forced with future Arctic sea ice loss

Box 4.4 Figure 1: Map of changes in the temperature of cold extremes (defined as the annual minimum of the daily minimum temperature) in Canada due to future Arctic sea ice loss relative to current conditions (1979–2008). The figure shows the multi-model average across 10 atmosphere-only models participating in the Polar Amplification Model Intercomparison Project. Future Arctic sea ice concentrations, which are prescribed in these experiments, correspond to concentrations at 2°C global warming above pre-industrial levels. Dots indicate where projected losses of Arctic sea ice significantly affect the temperature of cold extremes based on model simulations with and without Arctic sea ice loss. The dots indicate where the model difference is statistically significant at the 5% level (meaning there is a ≤ 5% chance of concluding that a difference exists when it does not).
Long description

The figure contains a map of Canada and the Northern United States showing how the temperature of cold extremes—defined as the coldest daily minimum temperature each year—is projected to change when Arctic sea ice is reduced to concentrations consistent with 2 °C of global warming.

Coloured shading across the map represents the multi model average change relative to the historical baseline period of 1979–2008. Warming of cold extremes (red shades) occurs across the map with greater warming around Hudson Bay and in Northern Quebec. Dots are overlaid on the shading and cover the entire map. The dots indicate locations where the difference between simulations with and without future Arctic sea ice loss is statistically significant.

4.3.3: Future changes

Climate models project that changes in the jet streams due to additional global warming will be small relative to internal climate variability, and will vary by season and region (C. Li et al., 2018; Oudar et al., 2020; Simpson et al., 2014). The IPCC AR6 WGI reported overall low confidence in projected regional changes in the Northern Hemisphere’s low-level west-to-east winds, particularly for the North Atlantic region in winter (Lee et al., 2021). Although there is a general tendency for a small poleward shift in both the Atlantic and Pacific jet streams, the magnitude of the shift is uncertain across individual models and seasons (Barnes & Polvani, 2013).

On average, climate models project a poleward shift in the jet streams and low-level west-to-east winds during spring and fall by the end of the 21st century under very high (RCP8.5) (Simpson et al., 2014) and intermediate (SSP2-4.5) emissions scenarios (Figure 4.9b,d). The projected shift shows better model agreement and is most pronounced during fall (Figure 4.9d). In summer, the Atlantic jet stream is projected to shift toward the North Pole while the Pacific jet stream is projected to weaken. In winter, the projected changes are more complex and uncertain. While the winter Pacific jet stream is projected to shift toward the North Pole, its eastern flank over the west coast of North America is projected to shift toward the equator, but with less model agreement (Figure 4.9a). The winter Atlantic jet stream appears to show only small changes with little model agreement (Figure 4.9a). However, these small apparent changes are a consequence of a robust poleward shift in early winter and an equatorward shift in later winter (García-Burgos et al., 2024).

Figure take-away: The jet streams are generally projected to shift toward the North Pole with additional climate warming, but this varies by season and region.

Figure title: Projected changes in low-level west-to-east winds

Figure 4.9: Maps showing projected changes in west-to-east wind speed across North America at 700 hPa (about 3 km above the Earth’s surface) in a) winter (December-January-February), b) spring (March-April-May), c) summer (June-July-August), and d) fall (September-October-November). The projections are based on CMIP6 multi-model averages for the late century (2081–2100) relative to the pre-industrial period (1850–1900). Wind speeds at this altitude in the atmosphere are an indicator of the strength of the jet stream. The grey contour lines indicate average wind speeds of 6 and 12 m/s for 1850 to 1900. The dots indicate where more than 90% of models agree on the sign of changes. Source: CMIP6 intermediate emissions scenario (SSP2-4.5).
Long description

This figure shows future projected changes in west to east wind speeds at 700 hPa—roughly 3 km above the surface—across North America for winter, spring, summer, and fall, based on a multi model climate simulation ensemble. Each panel displays the difference between late 21st century winds (2081–2100) and pre industrial conditions (1850–1900). Colours indicate how much winds are expected to strengthen or weaken: blue shades represent weaker westerlies, while yellow to red shades represent stronger westerlies, with grey contours every 6 m/s indicating the mean wind speeds under pre-industrial conditions. The black dots identify areas where more than 90% of the models agree on the direction of change, meaning these projected shifts are considered robust.

The maps reveal distinct seasonal patterns. Overall, the results highlight that the jet stream is expected to change differently by season, with notable changes in its strength and location under continued climate warming.

The uncertainty and large model spread in the response is in part due to the competing effects of upper and lower tropospheric temperature gradients (Oudar et al., 2020). In addition to model uncertainty, internal climate variability in the jet stream is expected to dominate over the forced response in near-term projections (Barnes & Polvani, 2015) and in projections at 1.5°C and 2.0°C warming (C. Li et al., 2018). Note that, except for fall, the projected trends in the jet stream over North America (Figure 4.9) appear different from the observed trends (Figure 4.8). These differences could be due to either model error or internal climate variability that has overwhelmed any forced trends. These discrepancies between observed trends and model projections contribute to the low confidence in both the projected responses and the attribution of the observed trend during these seasons.

Projected winter storm track changes are uncertain but show a small poleward shift, weakening over the Pacific and strengthening over the Atlantic by the end of the 21st century under intermediate (RCP4.5, SSP2-4.5) and very high (RCP8.5) emissions scenarios (Harvey et al., 2014, 2020). There is strong agreement across climate models that the summer storm tracks will weaken (have fewer or less intense storms or both) over North America and the mid-latitudes by the end of the 21st century under intermediate (RCP4.5, SSP2-4.5) and very high (RCP8.5, SSP5-8.5) emissions scenarios (E. K. M. Chang et al., 2016; Coumou et al., 2015; Harvey et al., 2020). However, there are disagreements on the amount that they weaken (Coumou et al., 2015), and the mechanism is not well understood (Kang et al., 2023).

Climate models generally project that the NAO and AO will shift toward their positive phases relative to the current climate, in all seasons except summer. The shift during winter is robust across most models under very high emissions scenarios (RCP8.5, SSP5-8.5) by the end of the 21st century, but there is strong disagreement across models in the magnitude that the NAO and AO will shift (Lee et al., 2021; McKenna & Maycock, 2021). In the near term (under all emissions scenarios) and for the end of the century under very low (SSP1-1.9) to intermediate (SSP2-4.5) emissions scenarios, the projected changes in the NAO and AO are relatively small compared to the magnitude of internal climate variability, and there is considerable spread across models (Lee et al., 2021). Models project little change in the AO during summer under all scenarios (Lee et al., 2021).

On average, climate models project little change in jet stream waviness, but with some spread across models and some dependence on season. A small decrease in jet stream waviness in the mid-troposphere over North America is projected for most seasons under high (SSP3-7.0) and very high (RCP8.5) emissions scenario by the end of the 21st century (Barnes & Polvani, 2015; Cattiaux et al., 2016; Nie et al., 2023; Yamamoto & Martineau, 2024). The projected decrease in waviness is more pronounced during summer and shows strong model agreement. In near-term projections, the changes in waviness are small compared to internal climate variability and model spread in all seasons (Barnes & Polvani, 2015). Overall, confidence in how jet stream waviness will change as the climate warms is low.

The low confidence in climate model projections of jet streams, storm tracks, and atmospheric modes of variability is due to weaknesses in models’ abilities to simulate observed changes and variability. This is particularly the case over the North Atlantic during winter where models appear to underestimate predictable signals in the NAO and the jet stream on seasonal timescales (Scaife & Smith, 2018), and underestimate variability on multidecadal timescales (Bracegirdle et al., 2018). The observed changes in the winter North Atlantic jet stream’s strength and NAO since the middle of the 20th century are also outside the ranges simulated by models, even after accounting for internal climate variability (Blackport & Fyfe, 2022). The reasons for these discrepancies between models and observations are not known, which means that their implications for the projections are uncertain.

4.3.4: Confidence terms in key messages: summary of evidence

Key message 4.3: Changes in recent decades in the jet streams and storm tracks that affect Canada are small and seen only in limited seasons and regions. There is low confidence in any human influence on these past changes. An overall poleward shift in the jet streams and storm tracks is projected by the end of the 21st century, but the changes are small and depend on the region and season (low confidence).

In short, we have low confidence in any human influence on changes in the jet streams, storm tracks, and atmospheric modes of variability that affect Canada. This assessment is based on the small magnitude of the trends compared to the large internal climate variability in most seasons and regions. In addition, climate models have difficulty capturing the past changes, making it challenging to understand the causes of those changes. The jet streams and storm tracks across Canada and the oceans around Canada are projected to shift poleward in a warming climate in some regions and seasons, but we have low confidence in such projections. This is because of disagreement across individual models, known model weaknesses, and a lack of understanding of the underlying physical mechanisms.

4.4: Extratropical storms and atmospheric blocks

Key message 4.4: Changes in recent decades in the frequency and intensity of extratropical storms and of atmospheric blocks are uncertain. There is low confidence in any human influence on these past changes. A poleward shift in extratropical storms and a decrease in the frequency of summer extratropical storms are projected over Canada (low confidence). Atmospheric blocks are projected to occur less frequently over Canada, but there are large regional variations (low confidence).

4.4.1: Effects on Canadian weather and climate

Extratropical cyclones are low-pressure weather systems occurring outside of the tropics. These are referred to as extratropical storms in this chapter. Their weather counterparts are extratropical anticyclones, which are referred to as extratropical high-pressure systems in this chapter. These extratropical storms and high-pressure systems are the dominant large-scale weather systems travelling across Canada. These weather systems typically travel from west to east with the jet stream. Strong extratropical high-pressure systems that persist over one region for several days or more are referred to as atmospheric blocks. The impacts of extratropical storms and atmospheric blocks on people, places, and nature depend on their intensity, their frequency, and their persistence or the speed at which they travel. Particularly strong extratropical storms and atmospheric blocks can bring extreme weather to Canada (Grotjahn et al., 2016; Yu et al., 2022). Atmospheric blocks, which result in strong distortions in the jet stream, are associated with both summer hot extremes (Figure 4.10) and winter cold extremes (Pfahl & Wernli, 2012). As an example, the June 2021 Pacific Northwest heatwave was associated with a particularly strong atmospheric block (White et al., 2023), creating atmospheric conditions that are sometimes referred to as a heat dome (Box 8.2).

Figure take-away: Atmospheric blocks can lead to surface heatwaves through multiple processes.

Figure title: Atmospheric blocks and heatwaves

Figure 4.10: Figure 4.10 presents a schematic representation of the processes that lead to surface heatwaves from atmospheric blocks. An atmospheric block occurs when a strong extratropical high-pressure system stays over one region for multiple days. Warm air builds up in the hot and typically dry conditions created by the atmospheric block. High pressure pushes warm air down toward the surface, which results in the air becoming compressed and heating up further, increasing surface temperatures. This warmer air also tends to create clear sky conditions as any cloud water evaporates. These clear skies result in an increase in downward shortwave radiation (i.e., an increase in heat from the sun reaching Earth), which further warms surface temperatures.
Long description

This figure illustrates a process where an atmospheric block over western North America alters the behavior of the jet stream, leading to a high-pressure event and associated warming at the surface. The visual trend shows how atmospheric blocking can lead to the buildup of heat by rerouting the jet stream, creating stagnant, clear skies and intensifying surface warming. Key visual elements include arrows indicating the diverted jet stream, the blocked region, and annotations tracking the flow from warm air accumulation to surface temperature rise. The image is annotated with six steps, describing how atmospheric blocking can lead to a heatwave. 1: Cooler air (of the jet stream) is deflected around a region of high pressure called an atmospheric block. 2: Warm air builds up in dry and hot conditions. 3: The high-pressure system pushes warm air downward towards the surface. 4: As air descends, it compresses and heats up even further. 5: Warm air leads to a decrease in cloud cover and produces clear sky conditions, letting more sunlight reach and heat the surface. 6: Downward shortwave radiation is increased due to clear skies, further warming surface temperatures, and often leading to heatwaves.

Strong extratropical storms can bring extreme precipitation and winds, as well as storm surges along the coasts (X. Zhang et al., 2023). These strong storms include explosive cyclones, also known as “bomb” cyclones, which intensify very rapidly, with a pressure drop of greater than 24 hectopascals (hPa, equivalent to millibars) within 24 hours (Sanders & Gyakum, 1980). Less frequent summer extratropical storms could lead to more persistent warm periods in summer (Coumou et al., 2015; Pfleiderer et al., 2019). Extratropical storms are more likely to form in certain locations and travel along certain pathways, creating storm track regions. Changes in extratropical storms can therefore result in changes in storm tracks, which are assessed in section 4.3. In this section, we assess changes from the individual storm perspective, including the frequency, strength, and movement of extratropical storms. Changes in extreme winds and rainfall associated with potential changes in extratropical storms are assessed in Chapter 8, section 8.4.3.

4.4.2: Past changes and their causes

Changes in extratropical storm frequency or intensity are studied using event-based tracking algorithms that detect, count, and track extratropical storms (e.g., Hoskins & Hodges, 2002). Methods to identify high-pressure systems are similar and often focus only on atmospheric blocks. The locations and movement of extratropical storms and high-pressure systems are strongly influenced by the jet streams and associated storm tracks. Changes in the frequency and intensity of extratropical storms and high-pressure systems can also be influenced by changes in temperature gradients and the extent of Arctic sea ice (Hay et al., 2023; T. Shaw et al., 2016) and changes in atmospheric moisture (Mathews et al., 2024). There is substantial uncertainty about, and low signal-to-noise ratios for, observed changes in extratropical storms, high-pressure systems, and atmospheric blocks (Gulev et al., 2021). Contributing to the uncertainty are low signal-to-noise ratios for observed changes in the jet streams and storm tracks (section 4.3), as well as the many complex and sometimes opposing mechanisms for potential changes in extratropical storms and high-pressure systems (T. Shaw et al., 2016; Steinfeld et al., 2022; Woollings et al., 2018). In addition, different tracking methods and different observational datasets can lead to differing trends for both extratropical storms (Neu et al., 2013; Walker et al., 2020) and high-pressure systems (Barnes et al., 2014; Woollings et al., 2018).

There is low confidence in observed trends for the frequency and strength of atmospheric blocks, even on a hemispheric scale, as trends vary widely depending on the reanalysis dataset, detection algorithm, and time period used (Barnes et al., 2014; Davini et al., 2012; Efe & Lupo, 2022; Lupo et al., 2019; Rohrer et al., 2019; Woollings et al., 2018). Trends in winter atmospheric-block frequency and intensity over Canada since the mid-20th century are weak (Davini et al., 2012; Woollings et al., 2018). Some evidence points to more frequent summer atmospheric blocks over eastern Canada since the mid-20th century (Woollings et al., 2018), but this increase is dependent on the blocking detection algorithm used (Pepler et al., 2019; Woollings et al., 2018). On longer timescales (since the early 20th century), the lack of agreement in trends between datasets gives low confidence in observed changes over Canada (Rohrer et al., 2019).

Observed changes in extratropical storm frequency vary by season and region, and also depend on the dataset and metric used to detect extratropical storms, resulting in low confidence in observed trends for Canada more broadly. There is some evidence for a past increase in Arctic storms over eastern Canada, although the trends vary with the time period (Neu et al., 2013; X. Zhang et al., 2023), season, and dataset used (Zahn et al., 2018). This potential past increase in Arctic storms is also consistent with an observed increase in atmospheric rivers (P. Zhang et al., 2023), although increases in atmospheric humidity, expected in a warming climate, can also explain the increase in atmospheric rivers (section 4.5). There is some evidence for an increase in strong extratropical storms during winter across southern Canada, and over the eastern Pacific and western Atlantic close to Canada (E. K. M. Chang & Yau, 2016; Douville et al., 2021). Across the Northern Hemisphere more broadly, studies find small increases in winter storm frequency (E. K. M. Chang & Yau, 2016; X. L. Wang et al., 2016), although even on a hemispheric scale this finding varies depending on the dataset used, leading to low confidence in these changes. These observed trends are also sensitive to the time period being analyzed, contributing to low confidence in attributing them to human activities (Rohrer et al., 2019; X. L. Wang et al., 2016). There is some evidence for a downward trend in the frequency of strong summer extratropical storms over the Northern Hemisphere, and particularly over eastern Canada and the western Atlantic (E. K. M. Chang et al., 2016). However, disagreement between reanalysis datasets and methodologies leads to low confidence in these trends (X. L. Wang et al., 2016). The observed decreases in summer extratropical storm frequency are consistent with decreases in the summer storm track strength over the Northern Hemisphere more broadly (section 4.3) (Chemke & Coumou, 2024). Recently, methods have been developed to quantitatively attribute strong extratropical storms to human-caused climate change, and there is some evidence that an increasing frequency of strong extratropical storms in Europe is due to human activities (Ginesta et al., 2023), but studies specifically for Canada are lacking.

4.4.3: Future changes

Overall, across the Northern Hemisphere, climate models project a decrease in the frequency of atmospheric blocks (Davini & D’Andrea, 2020; Lohmann et al., 2024; Matsueda & Endo, 2017; Woollings et al., 2018), including over parts of Canada. However, regional changes depend on the metric used to identify the atmospheric blocks, and fewer than two thirds of the CMIP5 models agree on the sign of the change over much of Canada (Figure 4.11). Both CMIP5 (Davini & D’Andrea, 2020) and CMIP6 models (Davini & D’Andrea, 2020; Lohmann et al., 2024) provide some evidence for a future small decrease in summer blocking over eastern Canada, although this is not consistent across all models and metrics (Gao et al., 2025). There is substantial disagreement in projected trends for winter between different models and metrics across Canada (Figure 4.11) (Gao et al., 2025; Jeong et al., 2023; Lohmann et al., 2024; Woollings et al., 2018). The lack of a complete theoretical explanation of how atmospheric blocks should respond to climate change (Hassanzadeh et al., 2014; Nabizadeh et al., 2019; Steinfeld et al., 2022; Woollings et al., 2018), combined with uncertainty about observed trends and climate model biases in the representation of atmospheric blocks (Davini & D’Andrea, 2016, 2020) leads to low confidence in projected changes over Canada.

Figure take-away: Projections of atmospheric-block frequency are very sensitive to the method used to identify atmospheric blocks and are inconsistent between different models, particularly for specific regions such as Canada.

Figure title: Projected changes in the frequency of atmospheric blocks in CMIP5 models for three different blocking metrics

Figure 4.11: Maps of rojected changes in winter and summer atmospheric-block frequency (2061–2090 relative to 1961–1990) over the Northern Hemisphere for three different blocking-detection methods (columns). The shading shows changes expressed as a percentage of days in the season; blue colours indicate lower frequency while red colours indicate higher frequency. These projections are based on the multi-model average of 25 CMIP5 models driven by a very high emissions scenario (RCP8.5). Changes are not shown for regions (in white) with a very low frequency of atmospheric blocks (< 1% of days in the season) in the historical period (1961–1990). Maps are oriented to be centred on the Arctic Ocean, with North America to the left of centre. In contrast to other figures in this chapter, dots show regions where there is a high level of disagreement between models, namely, where less than two thirds of the models agree on the sign of the change. The grey contour lines show the simulated frequency of blocking in the historical period, with each contour line depicting an increase in 2% of days in the season. Source: Woollings et al. (2018)
Long description

The figure contains six maps arranged in two rows and three columns showing projected changes in atmospheric‑block frequency over the Northern Hemisphere for winter (top row) and summer (bottom row) for the period 2061–2090 relative to 1961–1990 for a very high emissions scenario. Each column displays results using a different blocking‑detection methods.

The maps are centred on the North Pole and extend southward to a latitude of 30°N.  Shading indicates the projected change in blocking frequency as the percentage of days per season. Blue colours show decreased blocking; red colours show increased blocking. Regions shown in white had very low historical block frequency and therefore do not display projected changes. Black dots mark areas where fewer than two‑thirds of models agree on whether blocking increases or decreases, indicating high model disagreement. Grey contours are overlaid on the shading and depict historical blocking frequency in 2‑percent increments.

Overall, the maps show that projected changes vary widely by detection method, illustrating that atmospheric‑blocking projections—especially for regions such as Canada—are highly sensitive to methodological choices and inconsistent across models.

The projected poleward shift of the winter storm tracks in the North Pacific (section 4.3) is expected to lead to a poleward shift in the locations of winter extratropical storms (Lee et al., 2021), including explosive “bomb” cyclones (Seiler & Zwiers, 2016). This poleward shift will, in general, lead to an increase in the frequency of extratropical storms at higher latitudes, and a decrease at lower latitudes. In addition, there is some evidence that individual extratropical storms may travel further poleward under warming (Tamarin & Kaspi, 2017). Projected changes in the frequency of winter extratropical storms are small, particularly over Canada and the oceans around Canada (E. K.-M. Chang, 2018; Priestley & Catto, 2022a), with even the sign of the changes for specific regions dependent on the model or study methods or both (E. K.-M. Chang, 2018; Lee et al., 2021; Priestley & Catto, 2022b; Yettella & Kay, 2017; Zappa et al., 2013). Projected changes in the intensity of extratropical storms are also small (Seneviratne et al., 2012). For the summer season, climate models project a decrease in extratropical storm frequency for Canada and the oceans around Canada (E. K. M. Chang et al., 2016; Priestley & Catto, 2022a), consistent with the Northern Hemisphere average. This includes a weak response to Arctic sea ice loss (Kang et al., 2023). This projected decrease in frequency is also consistent with a projected weakening of the summer storm tracks (E. K. M. Chang et al., 2016; Harvey et al., 2020; Kang et al., 2023). There is also some evidence for a projected weakening of strong summer extratropical storms (Priestley & Catto, 2022a). Climate models have biases in the simulation of extratropical storms (Priestley et al., 2023), and disagree on many projections, particularly for specific regions, leading to low confidence in projections for Canada.

4.4.4: Confidence terms in key messages: summary of evidence

Key message 4.4: Changes in recent decades in the frequency and intensity of extratropical storms and of atmospheric blocks are uncertain. There is low confidence in any human influence on these past changes. A poleward shift in extratropical storms and a decrease in the frequency of summer extratropical storms are projected over Canada (low confidence). Atmospheric blocks are projected to occur less frequently over Canada, but there are large regional variations (low confidence).

The uncertainty about the observed changes of extratropical storm and atmospheric-block frequency and intensity over Canada is due to the sensitivity of observed trends to detection method and reanalysis dataset. Since the observed changes are small compared to internal climate variability, we have low confidence in attributing them to human influence. We have low confidence in projections that extratropical storms over Canada will shift poleward and become less frequent during summer, because of disagreement between individual models, known weaknesses in models’ abilities to simulate observed storms, including their changes and variability, and incomplete theoretical understanding. While models generally project a small decrease in the frequency of atmospheric blocks, there are large regional variations and a low level of model agreement, which results in low confidence in projections for Canada.

4.5: Atmospheric rivers

Key message 4.5: The frequency and intensity of atmospheric rivers have increased for Canada as a whole in recent decades (medium confidence). However, there is very low confidence in the magnitude of these increases due to the limited number of studies and the sensitivity of results to how atmospheric rivers are defined and detected. There is insufficient evidence to attribute long-term trends for Canada as a whole to human influence. However, human influence has increased the likelihood of extreme atmospheric-river events in southern British Columbia (low confidence). 

Key message 4.6: The frequency and intensity of atmospheric rivers over Canada will increase in the future in high emissions scenarios (high confidence) and intermediate emissions scenarios (medium confidence). However, the magnitude of these increases is uncertain.

4.5.1: Effects on Canadian weather and climate

Atmospheric rivers have emerged as an important research topic in recent decades, in part because they lead to weather and climate extremes when they make landfall (Guan et al., 2023; Newell et al., 1992; Ralph et al., 2004, 2017; Zhu & Newell, 1994, 1998). Atmospheric rivers are defined as corridors of strong water vapour transport that are thousands of kilometres long, up to a thousand kilometres wide, and transient, typically lasting one to three days. They are often associated with a low-level jet stream, typically around 1500 m above the surface, ahead of the cold front of an extratropical storm (AMS, 2024; Guan et al., 2023). Most atmospheric rivers are associated with an extratropical storm, and they therefore more frequently occur in regions where there are more frequent extratropical storms (Guo et al., 2020). The water vapour in atmospheric rivers can come from tropical or extratropical moisture sources, or some of both. It has been estimated that atmospheric rivers are responsible for more than 90% of poleward moisture transport across the mid-latitudes despite only occurring over around 10% of the Earth’s surface in these latitudes at any given time (Guan & Waliser, 2024; Zhu & Newell, 1998).

Atmospheric rivers can be observed directly with remote sensing (e.g., satellite measurements of water vapour) or during intensive field campaigns (e.g., using weather measurement devices called “dropsondes,” designed to be dropped from aircraft and to collect data as they fall to the Earth) (Ralph et al., 2004). However, observations have been limited in both their spatial and temporal coverage. Therefore, atmospheric rivers are typically detected using methods designed to identify their shape and structure in atmospheric reanalysis datasets or climate model outputs (Ralph, Wilson, et al., 2019; Shields et al., 2018). The resulting algorithm and reanalysis uncertainty is an important contributor to overall uncertainty when quantifying past and future change and the consequences of atmospheric rivers.

The major consequence of landfalling atmospheric rivers is persistent heavy precipitation, which can lead to extreme flooding, landslides, and avalanches. Some atmospheric rivers may cause damaging winds or dangerous Föhn wind events (relatively warm and dry downslope winds in the lee of mountain ranges) (Mo, 2024), or contribute to heatwaves (Bozkurt et al., 2018; Mattingly et al., 2023; Mo et al., 2022; Waliser & Guan, 2017). However, atmospheric rivers can also be beneficial by providing critical water supply for ecosystems and people (Ralph, Rutz, et al., 2019).

Figure take-away: Atmospheric rivers mostly affect the east and west coasts of Canada but can extend inland and be seasonally important in the north.

Figure title: Frequency of atmospheric rivers in Canada

Figure 4.12: Maps of a) annual and b) to e) seasonal atmospheric-river (AR) frequency (cumulative days per year or season in the ERA5 reanalysis with an atmospheric river detected) over Canada for the period 1940 to 2023. Atmospheric rivers are detected every six hours using a modified version (mtARget-v3) of the moisture-transport–based detection method of Guan and Waliser (2015, 2019). This version detects atmospheric rivers as contiguous regions of exceptionally strong moisture transport (where moisture transport exceeds the local, seasonally varying 85th percentile with a lower limit of 100 kg/m/s) that exhibit the characteristic geometry of an atmospheric river (length > 2,000 km and length-to-width ratio > 2). Source: Mo (2024).
Long description

The figure presents five maps of Canada and the nothern United States showing the frequency of atmospheric rivers (ARs) from 1940 to 2023. The first map shows annual AR frequency in days per year, while the other four maps show seasonal frequency—winter, spring, summer, and fall—expressed as days per season.

Coloured shading represents how many days per year or season ARs occur. In all maps, darker red colours indicate more frequent AR activity. Higher frequencies appear along the west coast—especially British Columbia—and the east coast, including Atlantic Canada and parts of Quebec.

Overall, the figure highlights that ARs predominantly affect coastal regions but occur throughout Canada, with notable seasonal variability and inland reach.

The presence and impacts of atmospheric rivers vary widely across Canada. In reanalyses for the period 1940 to 2023, atmospheric rivers are found to have occurred on average approximately 35 to 45 days per year (Figure 4.12a) (Mo, 2024) along both the west and east coasts of Canada. While most prevalent closest to the coasts, atmospheric rivers can extend inland. For example, atmospheric rivers have occurred, on average, between 20 and 35 days per year in Ontario and the Prairies, and 15 to 20 days per year in northern Canada. Atmospheric rivers are seasonally important in the Arctic, occurring 10 to 14 days per summer (Figure 4.12d), but less often in other seasons. The detection algorithm used in the analysis identifies atmospheric rivers on the basis of moisture transport thresholds. If an atmospheric river moving inland loses significant moisture, for example, as precipitation falls, to the point that it no longer meets the detection criteria, then it will fail to be classified as an atmospheric river. This pattern aligns with the physical nature of atmospheric rivers, which often weaken as they move away from their moisture sources.

Historically, atmospheric rivers affecting western Canada have received the most attention, in part because they interact with the region’s mountain ranges. Warm, moist marine airflow can be effectively blocked by the Pacific Coast and Rocky Mountain ranges in British Columbia, leading to prolonged and sometimes heavy rain falling on some windward mountain slopes. Intense atmospheric rivers contributed to the 2010 floods in the Bella Coola Valley, the massive snowstorm in mid-February 2015 in the Terrace-Kitimat Valley, and the catastrophic floods in southwestern British Columbia in mid-November 2021 (Gillett et al., 2022; Richards-Thomas et al., 2024). Based on a six-hourly atmospheric-river catalogue for the period 1948 to 2016, Gershunov et al. (2017) found that British Columbia and southeastern Alaska are hit by 30 to 40 landfalling atmospheric rivers each year on average, most of which occur during the fall and winter (Figure 4.12b–e). Atmospheric rivers contribute about 13% of total annual precipitation across these regions (Sharma & Déry, 2020a), with higher contributions (up to 33%) along the coast, including important contributions to streamflow (Sharma & Déry, 2020b). The higher coastal contributions are consistent with Gershunov et al. (2017), who found that about 30 to 40% of the annual precipitation in southwestern British Columbia can be attributed to landfalling atmospheric rivers.

Atmospheric rivers are also large contributors to annual precipitation along the east coast (Figure 4.13a) and are responsible for significant precipitation events in the Mackenzie River Basin (Gyakum, 2000; Smirnov & Moore, 1999, 2001). They also cause high-impact weather events in other parts of Canada, especially atmospheric rivers originating in the Gulf of Mexico and the Atlantic Ocean (Lin et al., 2019; Low et al., 2022; Mo & Lin, 2019; Mo, 2024; Newell & Zhu, 1994). A large proportion of moderate precipitation (Figure 4.13b) and wind extremes (Figure 4.13c) are associated with atmospheric rivers. Furthermore, in British Columbia, Quebec and southern Ontario, upwards of 70% of joint wind and precipitation extremes are associated with atmospheric rivers (Figure 4.13d). Note that Chapter 8 provides assessments of precipitation and wind extremes, including compound wind and rainfall events, which are relevant for infrastructure design.

Figure take-away: Atmospheric rivers contribute substantially to total precipitation, precipitation extremes, wind extremes, and compound precipitation and wind extremes in Canada.

Figure title: Contribution of atmospheric rivers to precipitation and wind extremes in Canada

Figure 4.13: Maps of a) the atmospheric-river (AR) contribution over Canada to annual precipitation totals from 1940 to 2023 and the association of atmospheric rivers with b) extreme precipitation events, c) extreme wind events, and d) events where both extreme precipitation and extreme winds happen at the same time. Extremes are defined as six-hour values whose magnitude equals or exceeds the top 2% of values for the period 1940 to 2023. The strength of the connection between atmospheric rivers and extremes is measured by looking at how often an atmospheric river occurs at the same time as these extreme events, compared to how often the extremes happen overall. Statistically significant associations with atmospheric rivers at the 5% level exist over the entire domain (meaning there is a ≤ 5% chance of concluding that an effect or trend exists when it does not). Source: Mo (2024)
Long description

The figure contains four maps of Canada and the northern United States showing how atmospheric rivers (ARs) contribute to different types of precipitation and wind events from 1940 to 2023. Coloured shading represents the percentage of events linked to atmospheric rivers.

The first map shows the AR contribution to annual total precipitation. Higher percentages, shown in blue, appear along the West and East Coasts, extending inland across British Columbia, Atlantic Canada and Quebec.

The second map shows the AR contribution to extreme precipitation events. Much of the West Coast of Canada shows strong AR influence, with elevated contributions also appearing in parts of Atlantic Canada.

The third map shows the AR contribution to extreme wind events. The highest contributions occur along the West Coast and adjacent interior regions.

The fourth map shows AR contributions to events where extreme precipitation and extreme winds occur at the same time. AR influence is strongest along the West and East Coasts. Overall, ARs contribute substantially to total precipitation, precipitation and wind extremes, and simultaneous precipitation and wind extremes in Canada.

4.5.2: Past changes and their causes

A water vapour corridor is considered an atmospheric river when its moisture transport reaches a certain strength. Its strength depends on the amount of water vapour in the atmosphere and on the direction and strength of winds that move this moisture from place to place. Changes in each of these factors will contribute to changes in atmospheric-river characteristics (Payne et al., 2020). According to the laws of thermodynamics (Box 8.3), human-caused climate change is expected to lead to increases in the amount of atmospheric moisture. For every degree-Celsius rise in temperature, air can hold around 6 to 7% more water vapour. Therefore, a warmer atmosphere can support more intense atmospheric rivers. Similar reasoning supports our understanding that precipitation driven by atmospheric rivers will intensify with warming (Payne et al., 2020). As noted in previous sections, however, there is generally less confidence in changes in winds, which are driven by atmospheric dynamics and the large-scale circulation.

The IPCC AR6 WGI concluded that it is likely there has been an increase in atmospheric-river activity in the eastern North Pacific since the mid-20th century, but it had low confidence in the exact magnitude of this trend, which has not been formally attributed to human-caused climate change. Still, the increase is in line with expected and observed rises in atmospheric moisture linked to human-caused global warming (Douville et al., 2021). A recent synthesis of multiple atmospheric-river detection algorithms and reanalyses (1980–2023) shows Canada-wide increases in atmospheric-river moisture and a global expansion of atmospheric-river area (Henny & Kim, 2025). Over western North America, observational and historical climate-modelling studies report increases in the occurrence of atmospheric rivers and of precipitation and streamflow associated with atmospheric rivers (Curry et al., 2019; Gershunov et al., 2017; Sharma & Déry, 2020c), with larger increases since the late 20th century (Sharma & Déry, 2020c). Trends estimated from multiple detection algorithms and reanalyses show robust increases in the frequency of atmospheric rivers over Atlantic Canada and the northern Pacific coast, accompanied by an intensification of moisture transport in the strongest atmospheric rivers (Henny & Kim, 2025). These results are consistent with up-to-date trends that show increases in the annual occurrence of atmospheric rivers and the intensity of the most extreme atmospheric rivers over North America since the middle of the 20th century (Figure 4.14).

Figure take-away: Atmospheric-river activity has increased over Canada since the mid-20th century.

Figure title: Past trends in annual occurrence of atmospheric rivers and in moisture transport during the strongest atmospheric river of the year

Figure 4.14: Maps of trends in a) annual atmospheric-river (AR) occurrence over Canada for 1940 to 2023, b) maximum instantaneous moisture transport during the strongest atmospheric river of each year, and c) total moisture transport over the duration of the strongest atmospheric river of each year. Statistically significant trends at the 5% level in annual atmospheric-river frequency (meaning there is a ≤ 5% chance of concluding that an effect or trend exists when it does not) are observed across much of Canada as indicated by the dots. The trends are expressed per century rather than per year. As an example, in a) a trend of 10 days per year per century is equivalent to an increase of 8.4 days per year over the 84-year period (1940–2023). Trends in moisture transport during the strongest atmospheric river of the year (panels b) and c)), show fewer areas with significant trends, but an overall pattern of increases in intensity over most of Canada. Source: Mo (2024).
Long description

The figure contains three maps showing past trends in atmospheric‑river (AR) activity across Canada from 1940 to 2023. All trends are expressed per century.

The first map shows trends in annual AR occurrence, measured as the number of AR‑affected days per year per century. Coloured shading ranges from blue (decreasing AR frequency) to red (increasing frequency). Much of Canada shows increases, with the largest upward trends in western Canada. Black dots overlaid on the shading cover most of Canada and mark locations where trends in AR frequency are statistically significant.

The second map shows trends in the maximum instantaneous moisture transport during the strongest AR of each year. The third map shows trends in the total moisture transport integrated over the duration of each year’s strongest AR.

These panels feature fewer statistically significant areas but still reveal increasing AR intensity in Western and Atlantic Canada.

Overall, the maps indicate that atmospheric‑river activity—both in frequency and intensity—has increased over Canada since the mid‑20th century.

Recent observational and modelling analyses have focused on regions outside of western North America, with findings that support those shown in figures 4.13 and 4.14. Dong et al. (2024) found upward trends in winter atmospheric-river frequency over eastern North America, including eastern Canada, in multiple reanalyses and high-resolution (∼50-km horizontal resolution) atmospheric model simulations. They attribute the upward trend in part to recent changes in the Pacific–North American teleconnection pattern (section 4.8), which also explain much of the interannual variability in the occurrence of atmospheric rivers. Studies focused on the Arctic have similarly emphasized the importance of year-to-year variability in modulating observed upward atmospheric-river trends. For example, Ma et al. (2024) found that regional differences in the expression of the Pacific Decadal Oscillation and the Atlantic Multidecadal Oscillation (section 4.8) are responsible for around a quarter of the variability in near-future spatially averaged Arctic atmospheric-river trends in climate model simulations. Studies that have split the observed increases in Arctic atmospheric rivers into thermodynamic and dynamical contributions have found that the thermodynamic contribution dominates (Ma et al., 2024; C. Zhang et al., 2023; P. Zhang et al., 2023). Overall, while upward trends in atmospheric rivers are found consistently for different regions of Canada across modern reanalyses, different detection algorithms describe their climatological characteristics—frequency, seasonality, and magnitude—in different ways (Collow et al., 2022), which can affect the magnitude of reported trends.

As concluded by the IPCC AR6 WGI (Douville et al., 2021), it has not been possible to assess the influence of human-caused climate change on long-term observed trends in atmospheric rivers or individual extreme atmospheric-river events, given the lack of formal attribution studies. (Note that Section 8.1.1 of the IPCC AR6 WGI report discusses the distinction between attribution of long-term trends in climate extremes and attribution for specific extreme events.) With some exceptions, this is still the case. One way to understand the causes of observed changes in atmospheric rivers is to use single-forcing climate model experiments, which evaluate the climate system’s response to individual classes of forcing agents, such as greenhouse gases or aerosols. Experiments of this type have found that the opposing effect of weakening influences from aerosols and strengthening influences from greenhouse gases led to modest historical change in atmospheric rivers over the west and east coasts of North America from 1920 to 2005 (Baek & Lora, 2021)Baek and Lora (2021). However, atmospheric rivers and precipitation driven by atmospheric rivers intensify rapidly in simulations for subsequent decades as the greenhouse gas signal starts to dominate. An event attribution study of the mid-November 2021 floods driven by atmospheric rivers over southwestern British Columbia found that human-caused climate change made the frequency of atmospheric-river events with similar storm-total moisture transport at least 60% more likely, made similar two-day precipitation 45% more likely, and made similar flooding 120 to 330% more likely (Gillett et al., 2022).

Atmospheric rivers can cause significant damage, including flooding, landslides, and destruction of infrastructure. An event in British Columbia in November 2021 resulted in an estimated Can$515 million in insured damages. Learn more about the economic impacts of atmospheric rivers and future flood scenarios in Section 5.3.3 of the British Columbia chapter of the Regional Perspectives Report, a report contributing to the Canada in a Changing Climate: National Assessment Process.

4.5.3: Future changes

Two main drivers of future changes in atmospheric rivers and atmospheric-river impacts over Canada can be attributed to human-caused climate change (Radić et al., 2015; Shields et al., 2023; S. Wang et al., 2023). The first, which affects atmospheric rivers globally, is the thermodynamically driven increase in moisture transport associated with the increase in water vapour that arises from the warming of the lower atmosphere. This increase in water vapour due to warming is also the primary driver of increases in precipitation and precipitation extremes associated with atmospheric rivers (Radić et al., 2015; Shields et al., 2023; S. Wang et al., 2023). The second is dynamically driven change, including the poleward shift in atmospheric rivers associated with a poleward shift in the mid-latitude storm tracks (section 4.3).

To illustrate these two main drivers, Figure 4.15 summarizes results from a recent model intercomparison project focused on assessing projected changes in atmospheric rivers in CMIP5 and CMIP6 climate models under very high emissions scenarios (RCP8.5, SSP5-8.5) (O’Brien et al., 2022). Simulated changes are broadly consistent with recent observed trends, indicating steady increases in the frequency of atmospheric rivers in the 21st century (Figure 4.15b) that are primarily driven by increases in atmospheric water vapour (Figure 4.15d). The dynamical component of change, which is attributed to the poleward shift in mid-latitude storm tracks (sections 4.3 and 4.4), reinforces this upward trend in the north and weakens it in the south (Figure 4.15e). Differences in how atmospheric rivers are defined and detected contributed as much to uncertainty as differences in climate models.

Figure take-away: Atmospheric rivers in Canada are projected to increase in frequency, mostly because of increases in atmospheric moisture.

Figure title: Projections of atmospheric-river occurrence and moisture transport

Figure 4.15: Maps of simulated historical frequency and changes in atmospheric rivers and their impacts on moisture transport across North America from a multi-model and multi–atmospheric-river (AR) detection method experiment. a) Historical (1981–2010) frequency of atmospheric rivers based on reanalysis data shows how often atmospheric rivers occurred in the past. b) Simulated changes (1951–2099), expressed as the trend in atmospheric-river days per year per century, suggest atmospheric rivers will occur more frequently under very high emissions scenarios (RCP8.5, SSP5-8.5). Trends are significant at the 5% level at all grid cells in the area shown (meaning there is a ≤ 5% chance of concluding that an effect or trend exists when it does not). c) Moisture transport by atmospheric rivers is expected to increase, meaning atmospheric rivers will carry more water vapour. d) This increase is largely driven by warmer air holding more moisture (thermodynamic effect). e) Changes in atmospheric circulation patterns (dynamical effect) also contribute to shifts in moisture transport, but to a lesser extent. The trends in b) to e) are expressed per century rather than per year. As an example, in b) a trend of 10 days per year per century is equivalent to an increase of 14.9 days per year over the 149-year period (1951–2099). Source: O’Brien et al. (2022).
Long description

The figure shows five maps illustrating past atmospheric‑river (AR) characteristics and projected changes across North America.

The first map shows the past frequency of atmospheric rivers from 1981–2010, based on reanalysis data. Coloured shading indicates how often ARs occurred, with the highest frequencies along the west and east coasts of North America and decreasing inland shown in red shading.

The second map shows the projected trend in AR frequency from 1951–2099, expressed as the change in AR days per year per century. Red shading indicates increasing AR frequency under very high emissions scenarios across North America.

The third map shows projected changes in total moisture transported by ARs and indicates that ARs are expected to carry more water vapour in the future.

The fourth map isolates the thermodynamic contribution to the changes in total moisture transported by ARs, showing that warmer air holding more moisture is the dominant cause of increased AR moisture transport.

The fifth map shows the dynamical contribution, reflecting changes in atmospheric circulation patterns. These circulation‑driven changes are smaller and tend to oppose the thermodynamic changes across most of North America except in parts of northern Canada and the Arctic.

Overall, the maps show that atmospheric rivers over Canada are projected to become more frequent and more moisture‑rich.

Evidence from studies based on different multi-model ensembles, across different generations of climate models (Gao et al., 2015; Hagos et al., 2016; Kolbe et al., 2023; Nellikkattil et al., 2023; Tan et al., 2020; M. D. Warner et al., 2015; P. Zhang et al., 2021; Zhao, 2020), show similar results. These results lead to high confidence that under high (SSP3-7.0) to very high (RCP8.5, SSP5-8.5) emissions scenarios, atmospheric rivers over Canada will increase in intensity and frequency, mainly because warming results in more moisture being transported (the thermodynamic driver). While studies with intermediate emissions scenarios are lacking, the same thermodynamic mechanism applies. Therefore, there is medium confidence that these results can be extrapolated to intermediate emissions scenarios, although the magnitude of changes will be smaller with less warming. The thermodynamic influence will also drive the intensification of atmospheric-river precipitation (Shields et al., 2023; S. Wang et al., 2023). However, the impact of changes in atmospheric circulation on changes in moisture transport, while smaller, adds to uncertainty about the overall magnitude of change. Uncertainty about the overall magnitude of change also arises from internal climate variability (Tseng et al., 2021), structural model uncertainty, and, as noted above for observed changes and by O’Brien et al. (2022), differences in how atmospheric rivers are defined and detected.

4.5.4: Confidence terms in key messages: summary of evidence

Key message 4.5: The frequency and intensity of atmospheric rivers have increased for Canada as a whole in recent decades (medium confidence). However, there is very low confidence in the magnitude of these increases due to the limited number of studies and the sensitivity of results to how atmospheric rivers are defined and detected. There is insufficient evidence to attribute long-term trends for Canada as a whole to human influence. However, human influence has increased the likelihood of extreme atmospheric-river events in southern British Columbia (low confidence). 

Key message 4.6: The frequency and intensity of atmospheric rivers over Canada will increase in the future in high emissions scenarios (high confidence) and intermediate emissions scenarios (medium confidence). However, the magnitude of these increases is uncertain.

Our medium confidence that the frequency and intensity of atmospheric rivers have increased over Canada since the mid-20th century is supported by evidence from multiple studies based on different reanalyses and using different methods of detecting atmospheric rivers. In addition, these reanalyses may be subject to inhomogeneity due to changes in the contributions of observational data sources over time. These trends are broadly consistent with historical climate model simulations, including single-forcing attribution experiments, as well as with our physical understanding of how atmospheric moisture increases with warming. However, we have very low confidence in the magnitude of trends and their attribution to human-caused climate change because of the lack of formal detection and attribution studies, the role played by internal climate variability, and the varying results depending on what atmospheric-river detection algorithm a study uses. There is insufficient evidence to attribute long-term trends for Canada as a whole to human influence as there are no studies that have addressed this. There is some evidence that human influence has increased the likelihood of extreme atmospheric-river events in southern British Columbia, but we have low confidence in this because the evidence is based on the attribution of only one recent atmospheric-river event.

Our high confidence in future increases in the frequency and intensity of atmospheric rivers over Canada under high (SSP3-7.0) and very high (RCP8.5, SSP5-8.5) emissions scenarios is supported by robust results from projections based on CMIP5 and CMIP6 simulations and using different climate models and atmospheric-river detection algorithms. These increases will be driven primarily by the increase in atmospheric water vapour associated with projected warming, which further supports our high confidence in projections of an intensification of heavy precipitation associated with atmospheric rivers. This is also consistent with our physical understanding. These changes (with a smaller magnitude) are also expected for intermediate emissions scenarios, but given the fact that there are no specific studies using intermediate emissions scenarios, we have only medium confidence in such projections. Our low confidence in the magnitude of changes stems from uncertainty about the influence of circulation changes. While of smaller magnitude, these changes are expected to play a role in modulating regional changes over Canada. Further uncertainty can be attributed to the internal climate variability, emissions scenario, climate model, and choice of atmospheric-river detection algorithm.

4.6: North Atlantic hurricanes

Key message 4.7: The strength and associated precipitation rates of North Atlantic hurricanes have increased (medium confidence). However, since only a small proportion of Atlantic hurricanes affect Canada, there is low confidence in the degree to which these changes have affected eastern Canada.

Key message 4.8: The average precipitation rates, maximum precipitation rates, and peak wind speeds associated with North Atlantic hurricanes, as well as the proportion of hurricanes in the North Atlantic that reach categories 4 and 5, are projected to increase (high confidence). However, regarding the small number of hurricanes affecting Canada, there is medium confidence in increasing precipitation rates and low confidence in increasing wind speeds. Changes in frequency of hurricanes affecting Canada are uncertain.  

4.6.1: Effects on Canadian weather and climate

Atlantic hurricanes are a subset of a weather phenomenon referred to as tropical cyclones. Tropical cyclones are low-pressure weather systems that, in contrast to the extratropical storms discussed in section 4.4, initiate over tropical oceans. The high sea surface temperatures in these tropical regions provide abundant energy for these cyclones to grow. Therefore, tropical cyclones can often grow to be much stronger, due to their lower pressure and thus faster winds, than extratropical storms. Although they are stronger, they are typically smaller in diameter. If a tropical cyclone has low enough pressure and fast enough winds to become sufficiently strong and evolves in the region around North America, it is called a hurricane. Hurricanes are categorized by strength, based on their pressure and wind speeds from 1 to 5, with 1 being the weakest that a cyclone can be while still being classified as a hurricane. Hurricanes typically form in the late summer and fall, and tend to move toward the northwest in the tropics, recurving toward the northeast if they travel north of 20 to 30°N (Knapp et al., 2010). As hurricanes move away from the warm tropical oceans, they weaken relatively quickly. The warm Gulf Stream temperatures along the east coast of North America can slow this weakening, allowing Atlantic hurricanes to occasionally reach Canada, in contrast to the cooler waters off the west coast, which prevent Pacific hurricanes from reaching the west coast of Canada. North Atlantic hurricanes can reach Canada either as tropical cyclones or as “post-tropical cyclones” (Milrad et al., 2009). A recent example of such a system is Hurricane Fiona, which made landfall over Nova Scotia as a post-tropical cyclone in 2022, impacting the entire Atlantic region. Other notable cyclones that made landfall over Canada in recent years as tropical or post-tropical cyclones include Hurricane Beryl (2024), Hurricane Dorian (2019), hurricanes Earl and Igor (2010), Hurricane Kyle (2008), and Hurricane Juan (2003). Given their intense winds and the related storm surge, hurricanes do not have to make landfall (defined as when the centre of the hurricane moves over land) to have damaging impacts in Canada.

Many, although not all, tropical and post-tropical cyclones weaken to below hurricane strength before they reach Canada. In fact, analysis of historical hurricane track datasets (IBTrACS, HURDAT2, NOAA Hurricane Research Division) (Knapp et al., 2010) shows that while Canada receives the remnants of tropical cyclones on average once or twice a year, it only suffers a direct hit by a tropical cyclone once every two years and a direct hit by a Category 1 or 2 hurricane once every three to four years. No major hurricane (Category 3, 4, or 5) has made landfall over Canada since reliable record-keeping began. When hurricanes do reach Canada, they bring strong winds and flooding due to both coastal storm surges and heavy precipitation. The Maritime provinces and the eastern part of Quebec are the regions most affected by tropical and post-tropical cyclones, although they have also affected southern Quebec (e.g., Hurricane Debby, in 2024) and even occasionally southern Ontario (e.g., Hurricane Hazel, in 1954).

4.6.2: Past changes and their causes

Detecting changes in tropical cyclones and attributing changes to human-caused climate change has been challenging. This is mainly because tropical cyclones occur relatively infrequently, and because it has been difficult to obtain precise and consistent data on tropical cyclones’ characteristics for climate research. Measurement systems have changed over time and have not always had comprehensive spatial coverage, particularly before the advent of Earth-observing satellites in 1979 (Kossin et al., 2013; Landsea et al., 2006). Globally, an increase in tropical-cyclone strength has been detected (Elsner, 2020; Emanuel, 2020; Kossin et al., 2020). This increase is consistent with the expected impact of human-caused warming based on theoretical considerations (Sobel et al., 2016) and high-resolution models (P. Chang et al., 2020; Knutson et al., 2020). While this increase in tropical-cyclone strength is also detectable at the basin level over the North Atlantic, no studies have investigated whether there is also an increase in hurricanes making landfall in Canada. A recent study reported an increase in tropical cyclone–related precipitation rates both at the global level and in the North Atlantic basin (Tu et al., 2021). Increasing precipitation rates have also been found for major Atlantic hurricanes making landfall in the continental United States (Touma et al., 2019). An increase in tropical cyclone–related precipitation is consistent with both our theoretical understanding of tropical cyclones and tropical cyclone-modelling studies. However, no studies have investigated whether an increase in precipitation is detectable in Canadian landfalling hurricanes. Some evidence suggests a shift toward an earlier start to the hurricane season in the North Atlantic region, which affects hurricanes making landfall in the United States in particular (Truchelut et al., 2022). There is also some evidence for a decrease in the dissipation rate of hurricanes after landfall for hurricanes forming in the North Atlantic (L. Li & Chakraborty, 2020), which, all else being equal, would allow hurricanes to reach further inland. These changes were primarily attributed to increasing sea surface temperatures. However, the small number of studies leads to low confidence in attributing changes in hurricane season’s start, or dissipation after landfall, to human-caused climate change, and it remains unclear whether there is a similar pattern for hurricanes that affect Canada. Estimates of North Atlantic hurricane size based on satellite or reanalysis data show no trends over the past several decades (Knaff et al., 2014; Schenkel et al., 2017; K. Zhang & Chan, 2023). An event attribution study of post-tropical cyclone Fiona (2022) found that human-caused climate change made the extreme wind speeds experienced over parts of Atlantic Canada during Fiona more than twice as likely when compared to the 1950–1979 climate (Malinina et al., 2025).

Hurricanes can cause significant damage to infrastructure, including healthcare facilities. Table 10.5 in Health of Canadians in a Changing Climate, a report contributing to the Canada in a Changing Climate: National Assessment Process, compiles information on the vulnerabilities of Canadian health facilities to specific climate change hazards, including hurricanes. It also contains examples of impacts on Canadian health facilities, including from flooding and extreme winds from hurricanes that have affected Canada

4.6.3: Future changes

The general consensus from theory and climate modelling is that, globally, the strongest tropical cyclones(in terms of low surface pressure and related wind speed) will get stronger in the future, and we should therefore expect an increase in the proportion of all tropical cyclones that reach very intense strength (Category 4 or 5) (Bhatia et al., 2018; P. Chang et al., 2020; Knutson et al., 2020; Patricola & Wehner, 2018; Roberts et al., 2020). At a global warming level of 2°C, the global strength of tropical cyclones is projected to increase by 5%, associated with a 13% increase in the proportion of all tropical cyclones that reach at least Category 4 (Knutson et al., 2020) These changes are projected to be accompanied by an approximately 15% increase in the precipitation rate of tropical cyclones, thus further increasing the chance of inland flooding. This projection agrees with the approximately 7% increase in atmospheric moisture per degree of warming required by physical theory (the Clausius-Clapeyron relationship). However, high-resolution climate modelling suggests that the precipitation rate near the inner core of the storms follows a “super Clausius-Clapeyron” scaling, with an increase in precipitation rates of 13 to 17% per degree of warming (M. Liu et al., 2019). While the confidence in these global changes is high, it is lower when extrapolating the changes to Canada because of other possible influences on regional scales and the small number of studies specifically on projections of hurricanes that affect Canada.

Projections of tropical-cyclone frequencies are not as robust as those associated with tropical-cyclone strength and tropical-cyclone precipitation because of the incomplete understanding of what determines the number of tropical cyclones, and the greater disagreement between models on projections of changes in frequency. For example, projections of tropical-cyclone frequencies for the North Atlantic basin are uncertain because the projected change in the annual number of tropical cyclones across different models and studies varies from minus 35% to plus 30% for a global warming level of 2°C, with a median value of minus 15% (Knutson et al., 2020). Confidence in such projections is further reduced by uncertainty about how the tropical equatorial Pacific, in particular the El Niño–Southern Oscillation (section 4.8), will respond to human-caused climate change, since changes in the tropical Pacific can influence the formation of Atlantic hurricanes (Sobel et al., 2023). Other changes in the characteristics of North Atlantic tropical cyclones, such as their size and amount of poleward propagation, could also lead to changes in tropical cyclones affecting Canada, but projections of such changes are currently uncertain (S. I. Seneviratne et al., 2021, Section 11.7.1). Tropical cyclones that do reach Canada may be influenced by changes in mid-latitude circulation, such as variations in the jet stream, which can affect extratropical transitions of hurricanes into post-tropical cyclones (Evans et al., 2017). Projected changes in the number of extra-tropical transitions remain uncertain, however, as most available evidence comes from single-model studies. Some of these studies suggest increases (A. J. Baker et al., 2022), while others indicate decreases (Cheung & Chu, 2023; M. Liu et al., 2017), and these changes are generally not statistically significant. Excluding any changes in Atlantic hurricanes themselves, increasing sea level due to human-caused climate change is projected to result in a larger influence of Atlantic hurricanes on extreme sea level events impacting coastal regions of Canada (Chapter 7, section 7.6) (Cheung & Chu, 2023)

4.6.4: Confidence terms in key messages: summary of evidence

Key message 4.7: The strength and associated precipitation rates of North Atlantic hurricanes have increased (medium confidence). However, since only a small proportion of Atlantic hurricanes affect Canada, there is low confidence in the degree to which these changes have affected eastern Canada.

Key message 4.8: The average precipitation rates, maximum precipitation rates, and peak wind speeds associated with North Atlantic hurricanes, as well as the proportion of hurricanes in the North Atlantic that reach categories 4 and 5, are projected to increase (high confidence). However, regarding the small number of hurricanes affecting Canada, there is medium confidence in increasing precipitation rates and low confidence in increasing wind speeds. Changes in frequency of hurricanes affecting Canada are uncertain.  

Our low confidence in past trends of hurricanes affecting Canada is due to the challenges of the changing observational system over the past decades, the relatively small number of events affecting Canada, and the lack of studies examining events affecting Canada specifically. We have medium confidence in increases in the strength and precipitation rates of North Atlantic hurricanes because some evidence exists for such increases and they are consistent with theoretical expected changes and changes on a global level.

We have high confidence that the strongest Atlantic hurricanes and their corresponding precipitation rates and peak wind speeds will intensify in the future. This is based on consistent evidence from theoretical understanding, observed changes, and model projections .

Regarding hurricanes affecting Canada, our medium confidence in projected increases in precipitation rates is due to the strong and well-understood effects of climate warming on tropical cyclone–related precipitation. We have low confidence in projected increases in wind speeds of hurricanes affecting Canada due to other possible influences on wind speeds on regional scales. Our lower confidence for both precipitation and wind speeds for Canada, relative to Atlantic hurricanes more broadly, is due to strong regional internal climate variability and the small number of studies specifically on projections of hurricanes that affect Canada.

Projected changes in the frequency of Atlantic hurricanes are uncertain due to a lack of established theory, multiple mechanisms through which changes could occur, a lack of understanding about the processes of possible changes, no clear observational signal, and disagreements between model projections. This leads to uncertainty about projected changes in the frequency of Atlantic hurricanes that affect Canada.

4.7: Large-scale environmental conditions favouring thunderstorms

Key message 4.9: There is low confidence that large-scale environmental conditions favouring thunderstorms in Canada have changed over the past several decades. This is due to a lack of regional studies for Canada, the weak, conflicting trends across different environmental-condition indicators and data products, and large internal climate variability.

Key message 4.10: Large-scale environmental conditions favouring thunderstorms are projected to become more prevalent across central and eastern Canada in spring, summer, and fall (high confidence). However, there is low confidence that thunderstorms and other severe weather events will increase, because an increase in favourable environmental conditions does not always lead to more thunderstorms.

4.7.1: Effects on Canadian weather and climate

Convective storms, which we refer to as thunderstorms for simplicity, are weather systems ranging from 2 to 200 km in scale that are associated with heavy rainfall caused by convection, the process by which warm and moist air rises, cools rapidly and produces rain through condensation. When thunderstorms are severe, they can also be associated with hail, strong winds, lightning, and tornadoes. Direct measurements of many of these phenomena can be limited, globally and in parts of Canada, and it is well-documented that storm reports are biased toward more densely populated regions, where there is a greater likelihood that a storm will be observed (Cheng et al., 2013; Etkin, 2018; Sills & Joe, 2019). For these reasons, it is sometimes difficult to establish reliable estimates of long-term trends in the occurrence of thunderstorms. In addition, global climate models lack sufficient granularity to simulate individual thunderstorms explicitly, making future thunderstorm occurrence uncertain. An alternative, indirect approach to estimating the occurrence of thunderstorms is to identify thunderstorm environments, consisting of key atmospheric conditions that favour the development of these storms (Brooks et al., 2003; R. H. Johns et al., 1993). The spatial distribution, severity, and frequency of such thunderstorm environments can be identified using atmospheric properties. Unlike thunderstorms themselves, which have relatively small spatial scales, thunderstorm environments tend to exhibit large-scale patterns of about 100 to 1000 km. It is important to note that conditions favourable to the development of thunderstorms do not always lead to their actual development, which is determined by processes that act on smaller scales than most climate models can simulate. Therefore, favourable conditions are indicators of thunderstorm environments but are not perfect predictors of actual thunderstorms. Furthermore, the correspondence between the indicators and actual thunderstorms varies depending on the region, season, or observational and reanalysis data product used, and may change as the climate warms (Gopalakrishnan et al., 2025; Hoogewind et al., 2017; Raupach et al., 2021; Tippett et al., 2019). In addition, changes in these indicators will not necessarily translate into changes in severe weather occurrences (Chapter 8, sections 8.3 and 8.4). However, there is value in assessing the changes in these indicators because they allow us to examine past changes consistently over time and give us some indication of how thunderstorms might change in the future using climate model output. This section assesses observed changes in and projections of thunderstorm environments, while Chapter 8 assesses observed changes in thunderstorm and severe weather events themselves.

One of the key atmospheric properties used as an indicator of thunderstorm environments is convective available potential energy, which is a measure of the instability of the atmosphere, that is, the capacity of the atmosphere to generate upward motion. Stronger convective available potential energy increases the amount of energy available for convection, which is essential for the development of thunderstorms. On the other hand, stronger convective inhibition (a measure of the energy that needs to be overcome for convection to occur) can prevent or delay the onset of convection. However, when combined with stronger convective available potential energy, convective inhibition can potentially increase the intensity of convection and associated precipitation (J. Chen et al., 2020; Del Genio et al., 2007; Diffenbaugh, N.S. et al., 2013; Rasmussen et al., 2017). Lower tropospheric vertical wind shear (the change in wind speed or direction that comes with a change in altitude) and storm relative helicity (a measure of the potential for cyclonic updrafts) are indicators of squall line or supercell development, with stronger shear and helicity leading to conditions that favour the development of more severe and longer-lived severe thunderstorms and tornadoes (Trapp, 2018). Thunderstorm environments are most often identified by combining several of these atmospheric properties together into what are called severe weather proxies (Lepore et al., 2021; Seeley & Romps, 2015). These atmospheric properties and severe weather proxies serve as indicators of the potential for severe weather, and their measurement and interpretation are crucial for forecasting such events (R. H. Johns & Doswell, 1992).

Atmospheric conditions that favour the development of thunderstorms, including tornadoes and hailstorms, are more prevalent in central and eastern Canada and in the Rocky Mountain region than in other parts of Canada (Figure 4.16a,c) (Brooks et al., 2003; Cheng et al., 2013; Etkin, 2018; Prein & Holland, 2018; Sills & Joe, 2019; Taszarek, Allen, Marchio, et al., 2021). Seasonally, thunderstorm environments in Canada are most prevalent in summer, followed by fall (Taszarek, Allen, Marchio, et al., 2021).

Figure take-away: Past trends in the frequency of conditions favourable to the occurrence of thunderstorms are weak across Canada.

Figure title: Past frequency and trends in the frequency of thunderstorm and severe thunderstorm environments in Canada

Figure 4.16: Maps of annual average climatology and past trends for a) and b) thunderstorm, and c) and d) severe thunderstorm environment frequency in Canada for 1979 to 2019. In c) and d), regions where trends are statistically significant at the 5% level (meaning there is a ≤ 5% chance of concluding that an effect or trend exists when it does not) are denoted with an “x” symbol. Thunderstorm environments (conditions favourable to the development of thunderstorms) are identified when convective available potential energy > 150 J/kg and convective precipitation > 0.25 mm/h and severe thunderstorm environments are identified as above but including an additional criterion that the vertical wind shear from the surface to 6 km > 12.5 m/s (Brooks, 2013). Data are from ERA5 reanalysis. Adapted from: Taszarek, Allen, Marchio, et al. (2021).
Long description

The figure contains four maps of Canada and the Northern United States arranged in two rows and two columns. The maps in the left column show coloured shading indicating the long-term average of the frequency of environments favourable for thunderstorms (top row) and severe thunderstorms (bottom row) in hours for the period 1979-2019.

For Canada, the highest frequencies occur in central and southern Canada.

The maps in the right column show coloured shading indicating the trend in the frequency of environments favourable for thunderstorms (top row) and severe thunderstorms (bottom row) in hours per decade over the same time period. Regions marked with an “x” overlaid on the shading have statistically significant trends. There are few “x”’s over Canada, indicating that past trends in the frequency of conditions favourable to the occurrence of thunderstorms are weak across Canada.

4.7.2: Past changes and their causes

Due to the limited number of regional studies that examine trends in thunderstorm environments in Canada, there is low confidence that thunderstorm environments in Canada have changed over the past several decades. This low confidence is also due to small and conflicting trends across different atmospheric properties, severe weather proxies, and data products.

Many studies examining past trends in thunderstorm environments focus on the continental United States (Koch et al., 2021; Taszarek, Allen, Brooks, et al., 2021). While some information can often be gleaned from these studies for the southernmost regions of Canada, it is not possible to extrapolate to the rest of Canada. Moreover, different studies use different proxies and different data products, making it challenging to compare and assess past changes (J. Chen & Dai, 2023; F. Li et al., 2020; Pilguj et al., 2022; Tang et al., 2019; Taszarek, Allen, Marchio, et al., 2021).

With respect to conflicting trends, observed trends for convective available potential energy in Canada display differing trends in in-situ observational data and reanalysis data in some regions of Canada (J. Chen & Dai, 2023; F. Li et al., 2020; Pilguj et al., 2022; Taszarek, Allen, Marchio, et al., 2021). Furthermore, relatively weak and spatially heterogeneous trends have been observed in thunderstorm environments in Canada for 1979 to 2019 (Taszarek, Allen, Marchio, et al., 2021), while upward trends in hailstorm environments have been observed for southeastern Canada (A. W. Johnson & Sugden, 2014; Tang et al., 2019). Finally, observations indicate lightning has increased in western and northern Canada and decreased in central and eastern Canada in recent decades (Burrows et al., 2025; Kochtubajda & Burrows, 2020), but these results do not align with trends in thunderstorm environment frequency (Figure 4.16b,d).

The inconsistency across severe weather proxies may be due in part to opposing changes in the properties of thunderstorm environments. Theory suggests that as the climate warms, the atmosphere will become more unstable over land areas, meaning that convective available potential energy will increase. On the other hand, convective inhibition will also increase and vertical wind shear in the lower troposphere will likely decrease (Seeley & Romps, 2015; Singh & O’Gorman, 2013; Trapp et al., 2007). These opposing changes, in addition to large internal climate variability, make it challenging to detect trends in thunderstorm environments for the recent past (Franke et al., 2024).

In this section, the assessment has been limited to past changes in thunderstorm environments. For details on changes in the storms themselves and associated short-duration precipitation, hail, and strong winds, see Chapter 8, sections 8.3 and 8.4, respectively.

4.7.3: Future changes

Climate model projections show an overall increase in the prevalence of environmental conditions that favour thunderstorm development in Canada (Diffenbaugh, N.S. et al., 2013; Gensini et al., 2014; Glazer et al., 2021; Lepore et al., 2021; Rasmussen et al., 2017; Raupach et al., 2021). Models project an increase in Canada of such favourable environmental conditions ranging from 40 to 53% per degree Celsius of global warming (Figure 4.17). The prevalence of thunderstorm environments is projected to increase across southcentral and eastern Canada in all seasons, with spring showing the largest percentage increases (Lepore et al., 2021). Thunderstorm environments are projected to extend further north in central and eastern Canada and into the Northwest Territories and Nunavut in summer, despite greater opposition between increases in convective available potential energy and decreases in vertical wind shear in the lower troposphere in this region (Lepore et al., 2021; Paquin et al., 2014). The winter season is not shown because there are too few occurrences of thunderstorm environments during the past several decades to robustly assess relative future changes.

The increase in conditions favourable to the development of thunderstorms is mainly due to thermodynamic processes: a strong increase in convective available potential energy (high confidence) as the climate warms that is not fully opposed by increasing convective inhibition (J. Chen et al., 2020; Diffenbaugh, N.S. et al., 2013; Lepore et al., 2021; Seeley & Romps, 2015; Singh & O’Gorman, 2013). An increase in moisture in the lower atmosphere due to climate change is an important factor driving increases in convective available potential energy, while a decrease in relative humidity in the lower atmosphere over land contributes to greater convective inhibition (Byrne & O’Gorman, 2016; J. Chen et al., 2020; Diffenbaugh, N.S. et al., 2013; Rasmussen et al., 2017). Regional climate model projections with sufficient granularity to simulate convection show that the combination of stronger convective available potential energy and stronger convective inhibition has the potential to suppress mild and weak storms but to generate more extreme storms with more intense rainfall (Dai et al., 2017; Prein et al., 2017; Rasmussen et al., 2017). Dynamical processes that affect storm organization and severity, vertical wind shear, and helicity show relatively weak decreases (Diffenbaugh, N.S. et al., 2013; Lepore et al., 2021; Seeley & Romps, 2015).

Figure take-away: The frequency of the environmental conditions favourable to the occurrence of thunderstorms in Canada increases with increasing global warming levels.

Figure title: Percentage increases in the frequency of thunderstorm environments in Canada as a function of global warming level

Figure 4.17: Graphs of seasonal, multi-model percentage change of favourable thunderstorm environment frequency relative to the historical period (1980–2015) weighted for Canada as a function of global warming level (coloured bold lines). Thunderstorm environments are quantified based on the average of seven different severe weather proxies. Vertical lines indicate global warming levels of 1°C, 1.5°C, 2°C, and 3°C relative to the preindustrial period (1850–1900). Text located on the vertical lines indicates the percentage change projected for that specific temperature increase. Seasons are spring (March-April-May), summer (June-July-August), and fall (September-October-November). Shaded areas represent the intra-model and intra-proxy 95% confidence intervals. Linear fit (coloured, solid straight lines) and the 95% confidence interval (coloured dashed lines) are fit to a 0.8–3°C interval. Bold text on the top left of each panel represents the percentage change per degree Celsius increase in global temperature based on the linear fit. Adapted from: Lepore et al. (2021).
Long description

The figure consists of three side by side panels showing how the frequency of favourable thunderstorm environments in Canada is projected to change with increasing global warming. Each panel corresponds to a season: Left panel: spring, middle panel: summer, and right panel: autumn. Dashed vertical lines in each panel mark global warming levels of 1 °C, 1.5 °C, 2 °C, and 3 °C.

The vertical axis shows percentage change relative to the historical period of 1980–2015. The horizontal axis shows global warming level from 0 to 4 °C above pre industrial conditions. In each panel, a coloured bold curve traces the multi model average percentage change based on the average of seven severe weather proxies. These curves are all oriented on a diagonal from the lower left to upper right indicating increasing percentage change with global warming level. Shaded regions of the same colour as each bold line represent the 95% confidence interval across the models and proxies. A straight coloured line in each panel shows the linear fit and matching dashed lines show its 95% confidence interval. Large bold numbers at the top left of each panel indicate the percentage change per degree Celsius of global warming based on the linear fit.

Overall, climate model projections show increasingly favourable environmental conditions for thunderstorm development. However, the IPCC AR6 WGI concluded (Seneviratne et al., 2021, Section 11.7.3.5) that there is generally low confidence in projections of changes in thunderstorms based on thunderstorm environments because the relationship between simulated thunderstorm environments in models and the occurrence of observed thunderstorms requires improved validation and may change as the climate changes. Moreover, recent analysis indicates that model biases in key atmospheric properties, such as convective available potential energy, can lead to uncertainty in estimates of the prevalence of thunderstorm environments in models, contributing to the low confidence assessment (Gopalakrishnan et al., 2025).

4.7.4: Confidence terms in key messages: summary of evidence

Key message 4.9: There is low confidence that large-scale environmental conditions favouring thunderstorms in Canada have changed over the past several decades. This is due to a lack of regional studies for Canada, the weak, conflicting trends across different environmental-condition indicators and data products, and large internal climate variability.

Key message 4.10: Large-scale environmental conditions favouring thunderstorms are projected to become more prevalent across central and eastern Canada in spring, summer, and fall (high confidence). However, there is low confidence that thunderstorms and other severe weather events will increase, because an increase in favourable environmental conditions does not always lead to more thunderstorms.

In summary, we have low confidence in observed changes in the prevalence of thunderstorm environments in Canada. This assessment is based on a lack of regional studies for Canada; large atmospheric internal climate variability; and weak and conflicting trends across different data products, severe-weather proxies and individual properties that contribute to the prevalence of thunderstorm environments. We have high confidence in an increase in convective available potential energy as the climate warms, resulting in an increase in the prevalence of favourable thunderstorm environments across central and eastern Canada in spring, summer, and fall. This assessment is based on theoretical understanding of how convective available potential energy will change as the climate warms. It is also based on multiple studies using global climate model projections with regional climate model projections that have sufficient granularity to simulate thunderstorms. However, in line with the assessment by the IPCC AR6 WGI, we have low confidence that increases in the frequency of these environments will translate into increases in thunderstorms themselves. This assessment is based on uncertainties in the accuracy and stationarity of severe weather proxies used to identify thunderstorm environments, climate model biases in the simulation of key properties that contribute to thunderstorm environments, and the fact that global climate models do not have sufficient granularity to simulate thunderstorms.

4.8: El Niño–Southern Oscillation and other atmosphere-ocean coupled modes of variability

Key message 4.11: The El Niño–Southern Oscillation (ENSO) is the dominant source of year-to-year climate variability in western Canada. Year-to-year climate fluctuations associated with ENSO have been larger since 1950 than in the previous century (medium confidence). However, there is low confidence that this change is due to human-caused climate change because internal climate variability is large.

Key message 4.12: The El Niño–Southern Oscillation (ENSO) will remain the dominant source of climate variability in western Canada in the 21st century (high confidence), but there is low confidence in projected changes in year-to-year climate fluctuations associated with ENSO. While climate models consistently show that by the end of the century, the effect of ENSO on winter climate fluctuations will extend into central and eastern Canada, there is low confidence in these projections due to systematic climate model biases.

4.8.1: Effects on Canadian weather and climate

Atmosphere-ocean coupled modes of climate variability are oscillations or fluctuations that involve the interaction or coupling between sea surface temperatures and the atmosphere, leading to local and remote large-scale atmospheric circulation anomalies that can influence climate and weather across large distances. The remote atmospheric circulation anomalies are often termed “teleconnections” and can directly affect surface temperature and precipitation in Canada. The dominant atmosphere-ocean coupled modes of climate variability affecting Canada are the El Niño–Southern Oscillation (ENSO) (Philander, 1990), the Pacific Decadal Oscillation (PDO) (Mantua et al., 1997), and the Atlantic Multidecadal Oscillation (AMO) (Kerr, 2000). Brief definitions of these modes can be found in Box 4.1.  

ENSO is the dominant mode of year-to-year climate variability in western Canada and originates from coupled atmosphere-ocean interactions in the tropical Pacific (Philander, 1990). It is characterized by fluctuations in sea surface temperature with warmer than average (El Niño) and colder than average (La Niña) sea surface temperatures in the central to eastern equatorial Pacific occurring every two to seven years. The ENSO amplitude (or strength) is the magnitude of these fluctuations. It is typically quantified by the anomaly (the difference relative to average conditions) of the sea surface temperature in a rectangular region of the central tropical Pacific, such as the Niño 3.4 region, within 5oN to 5oS and 120oW to 170oW. Larger positive (warmer than average) or negative (cooler than average) sea surface temperature anomalies in the central tropical Pacific indicate stronger El Niño or La Niña events, respectively. ENSO is associated with anomalies in tropical atmospheric deep-convection and heating, leading to the formation of atmospheric teleconnections affecting climate on a global scale (e.g., Timmermann et al., 2018; Trenberth et al., 1998; Yeh et al., 2018). ENSO influences temperature and precipitation in Canada mainly through an atmospheric teleconnection that resembles the Pacific–North American teleconnection pattern (PNA), (Wallace & Gutzler, 1981). The effects of this teleconnection are most pronounced in the winter season (Ropelewski & Halpert, 1986). Climate anomalies associated with the warm (positive) phase of ENSO (El Niño) are shown in Figure 4.18. During El Niño events, a positive PNA-like pattern is typically observed. This pattern moves warm southern air northward into western and central Canada, resulting in warmer winter air temperatures and drier conditions across much of southern Canada. When this happens, warmer than average temperatures are most prominent in western and central parts of southern Canada, while drier than average weather is most prominent in southwestern Canada (Figure 4.18, top panels). Generally, opposite patterns are observed during La Niña events, although some asymmetries exist (e.g., Burgers & Stephenson, 1999; Eyring et al., 2021a; Hayashi et al., 2020). The strength of the temperature and precipitation anomalies are influenced by ENSO amplitude. ENSO has little impact on summer temperature and precipitation variations in Canada.

ENSO events are divided into two types, eastern and central Pacific, whose names indicate the location of the largest sea surface temperature anomaly during the event (Ashok et al., 2007; Capotondi et al., 2015). Different types of events tend to produce distinct large-scale teleconnections and remote climate effects (e.g., Ratnam et al., 2014; Taschetto et al., 2020). The effects on Canadian temperature and precipitation are slightly weaker for central Pacific ENSO compared to eastern Pacific ENSO events, as the teleconnected circulation responses are slightly weaker and shifted westward (Yu et al., 2015).

The PDO is the result of a combination of physical processes across the tropics and extratropics, including remote tropical forcing—primarily from ENSO—and local North Pacific atmosphere-ocean interactions (e.g., Newman et al., 2016; Schneider & Cornuelle, 2005). The spatial pattern of the PDO resembles that of ENSO, but the amplitude of the sea surface temperature anomalies associated with the PDO is larger in the mid-latitudes (Figure 4.18, middle left panel). The largest distinction between the PDO and ENSO is their timescales: ENSO is primarily a phenomenon that varies irregularly over periods of a few years, while the PDO varies irregularly over timescales ranging from years to decades. The PDO also influences Canadian climate through PNA-like teleconnections. However, the centre of action of the PDO-associated atmospheric circulation anomalies is further west and north than those associated with ENSO. As a result, a positive PDO phase usually brings warmer than average temperatures to western and northern Canada and drier than average conditions to southwestern Canada (Figure 4.18, middle panels).

Figure take-away: Atmosphere-ocean coupled modes of climate variability (El Niño–Southern Oscillation, Pacific Decadal Oscillation, and Atlantic Multidecadal Oscillation) influence the prevailing winter climate conditions in Canada.

Figure title: Winter climate anomalies associated with positive phases of the El Niño–Southern, Pacific Decadal, and Atlantic Multidecadal oscillations from 1951 to 2022

Figure 4.18: Maps of winter climate anomalies—defined as differences relative to average conditions—associated with the positive phase of the El Niño–Southern Oscillation (ENSO) (top row), Pacific Decadal Oscillation (PDO) (middle row), and Atlantic Multidecadal Oscillation (AMO) (bottom row). Anomalies are opposite for the negative phase. This figure illustrates how sea surface temperature (SST) anomalies and the resulting teleconnected atmospheric circulation anomalies (left column) lead to temperature and precipitation anomalies in Canada in winter (middle and right columns). Solid and dashed contours indicate positive and negative anomalies in metres in the 500 hPa height (Z500), corresponding to clockwise and counterclockwise atmospheric-circulation anomalies. Colours indicate SST anomalies in degrees Celsius (left column), surface air temperature (SAT) in degrees Celsius (middle column), and precipitation in millimetres per day (right column). Red colours indicate warmer than average, blue colours colder than average, brown colours dryer than average, and green colours wetter than average conditions.  Results are based on linearly detrended ERA5 reanalysis data for 72 winters (December-January-February) from 1951 to 2022. Anomalies are calculated by relating the data to the time series of the corresponding index and dividing by their standard deviation. The ENSO index used is the Niño 3.4 index, which represents SST anomalies in the Niño 3.4 region (5°N–5°S, 120°W–170°W). Dots indicate anomalies that are statistically significant at the 5% level (meaning there is a ≤ 5% chance of concluding that an effect or trend exists when it does not). Data source: The Niño 3.4, PDO and AMO indices were obtained from datasets maintained by the National Oceanographic and Atmospheric Agency, available at Climate Indices: Monthly Atmospheric and Ocean Time Series.
Long description

The figure consists of nine maps arranged in three rows and three columns. Each row represents the winter climate anomalies associated with one major climate mode: (top row) the positive phase of the El Niño–Southern Oscillation (ENSO), (middle row) the Pacific Decadal Oscillation (PDO), and (bottom row) the Atlantic Multidecadal Oscillation (AMO).  In the left column, maps show sea surface temperature anomalies (SST) in degrees Celsius for latitudes ranging from 20S to 90N and longitudes ranging from 120E to 0 using coloured shading. Red shading indicates warmer than average SSTs, and blue shading indicates cooler than average SSTs.

For ENSO (top row), the dominant feature is warm SST anomalies in the western tropical Pacific. For the PDO (middle row), the dominant feature is a semi-circular pattern of warm SST anomalies extending north from the western tropical Pacific along the coast of western North America. For the AMO (bottom row), the dominant feature is warm SST anomalies  in the North Atlantic.

For each map, solid contours are superimposed on the shading and represent positive 500 hPa height anomalies (Z500), indicating anomalous clockwise atmospheric circulation, while dashed contours indicate negative Z500 anomalies, representing counterclockwise circulation.

For ENSO and the PDO (top and middle rows), the dominant feature is a counterclockwise circulation in the North Pacific. For the AMO (bottom row), the dominant feature is a clockwise circulation in the North Atlantic.

In the middle column, maps of Canada show surface air temperature anomalies in degrees Celsius using coloured shading. Red shading indicates warmer than average winters; blue shading indicates cooler-than-average. The spatial patterns vary by climate mode (rows). Regions with dots overlaid on the shading indicate where anomalies are statistically significant.

For ENSO (top row), statistically significant warm anomalies  cover most of southern Canada and northwestern Canada. For the PDO (middle row), statistically significant warm anomalies  stretch from western Canada to Hudson’s Bay, decreasing in magnitude from west to east. For the AMO (bottom row), statistically significant warm anomalies  cover most of Quebec, northern Ontario and the southeastern Northwest Territories.

In the right column, maps of Canada show precipitation anomalies in millimetres per day using coloured shading. Brown shading indicates drier than average conditions, and green shading indicates wetter than average conditions. The spatial patterns vary by climate mode. Regions with dots overlaid on the shading indicate where anomalies are statistically significant.

For ENSO and the PDO (top and middle rows), statistically significant wet anomalies occur in coastal (PDO) and southwestern British Columbia (ENSO), while dry anomalies  cover the Yukon, British Columbia, Alberta and Saskatchewan. For the AMO (bottom row), there are no statistically significant wet or dry anomalies.

The AMO is a pattern of interdecadal (every ten years or so) to multidecadal (every few decades) variability characterized by North Atlantic sea surface temperature fluctuations (Kerr, 2000), with a characteristic timescale of 60 to 80 years. It features sea surface temperature anomalies across most of the North Atlantic, with stronger anomalies in the subpolar region and weaker anomalies in the tropics (Figure 4.18, lower left). The AMO is the result of slowly varying ocean processes, whereas the atmospheric North Atlantic Oscillation (described in section 4.3) varies on shorter, interannual (every few years) and even shorter timescales. However, the AMO affects climate in eastern Canada primarily through teleconnections that are like the North Atlantic Oscillation, except that they are shifted westward. During the positive phase of the AMO, a negative North Atlantic Oscillation–like pattern is typically observed, which corresponds to weaker than average west-to-east winds. Relative to average conditions, there is more transport of relatively warm ocean air into eastern Canada, causing warmer than average temperatures in the eastern parts of the country. The impact of the AMO on Canadian precipitation is generally weak (Figure 4.18, lower panels).

Due to its relatively long timescales, ENSO can be predicted months to years in advance, which helps predict climate patterns across Canada on seasonal to annual timescales (see also Chapter 3, section 3.4.1). The PDO can be predicted with moderate skill, while the AMO is somewhat predictable on decadal to multidecadal timescales and is important for understanding long-term climate variability across eastern Canada (Chapter 3, section 3.4.1). It is important to note, however, that the specific effects of ENSO, PDO, and AMO may vary from event to event, and that teleconnections can interact with each other.

4.8.2: Past changes and their causes  

Observations reveal strong multidecadal variations in both the amplitude and frequency of ENSO events throughout the 20th century (e.g., Gulev et al., 2021; Hope et al., 2017; J. Li et al., 2013; Torrence & Compo, 1998). The amplitude of ENSO has been high in recent decades but was relatively low in the mid-20th century (Gulev et al., 2021). Increased ENSO amplitude has the potential to increase associated year-to-year variations in temperature and precipitation in Canada. However, because of short observational datasets and large internal climate variability, such changes in year-to-year variability have not been identified. On the longer timescales, the IPCC AR6 WGI (Gulev et al., 2021) found that there is medium confidence that both ENSO amplitude and the frequency of high-magnitude events since 1950 are higher than they were over the previous century. Observations also show an increase in the number of central Pacific ENSO events in last 20 to 30 years (Capotondi et al., 2015; McPhaden et al., 2011; Timmermann et al., 2018).

There is no clear evidence that the observed changes in ENSO amplitude and event type can be attributed to human-caused climate change (Eyring et al., 2021a; L’Heureux et al., 2013). Climate model simulations do not show strong trends in ENSO amplitude over the past decades and show large internal climate variability, suggesting that observed trends are the result of internal climate variability and are unrelated to human-caused climate change (e.g., Hope et al., 2017; N. Maher et al., 2018; Stevenson et al., 2019). By contrast, there is some evidence that natural and human-caused climate forcings have contributed to variability resembling the PDO and AMO. For example, climate model simulations suggest that the PDO is affected by large volcanic eruptions and changes in incoming solar radiation, both of which are natural climate forcings (e.g., T. Wang et al., 2012). Modelling experiments also suggest that past changes in aerosols from human activity have influenced the phase of the PDO (Boo et al., 2015; Dittus et al., 2021; Klavans et al., 2025), although there is a large degree of uncertainty about such an influence due to large internal climate variability (Oudar et al., 2018). Human-caused greenhouse gases (Bellomo et al., 2018; Mann & Emanuel, 2006; Murphy et al., 2017), human-caused aerosols (Booth et al., 2012; Qin et al., 2020), and volcanoes (Mann et al., 2021) have all been linked to changes in the phase of the AMO. However, no consistent trends in the PDO and AMO have occurred over the historical period (high confidence).

4.8.3: Future changes

The IPCC AR6 WGI report assessed there is high confidence that ENSO will remain the primary mode of climate variability in the 21st century (Lee et al., 2021). The report also found that there is no robust model consensus on changes in ENSO amplitude and ENSO type frequency during the 21st century with warming, even under very high emissions scenarios (SSP5-8.5, RCP8.5) (Bellenger et al., 2014; W. Cai et al., 2018, 2022; Freund et al., 2020; Lee et al., 2021; Wengel et al., 2021). However, it also found that climate models project a significant increase in the strength of precipitation variations associated with ENSO over the 21st century under all emissions scenarios, with larger increases for higher emissions scenarios (Lee et al., 2021; Power et al., 2013; Yun et al., 2021). ENSO-related precipitation variations are also projected to shift and extend eastward under global warming (Huang & Xie, 2015; Power et al., 2013; Yan et al., 2020). These changes modulate teleconnections, resulting in changes in the effects of ENSO on remote temperature and precipitation variations (Beverley et al., 2021; Brown et al., 2020; Taschetto et al., 2020; Y. Wang et al., 2022). On average, CMIP6 models project that Canadian temperature and precipitation variations associated with ENSO will expand eastward (Figure 4.19). These changes are associated with climate models projecting greater warming in the eastern compared to the central tropical Pacific, which reduces the sea surface temperature difference across this region and causes the teleconnections to shift eastward. However, confidence in these climate model projections is limited due to systematic model biases in the simulations of the tropical Pacific. Observations show a persistent cooling of the eastern equatorial Pacific in recent decades, while climate models show a persistent warming (Bayr et al., 2019; Coats & Karnauskas, 2017; N. C. Johnson et al., 2019; L’Heureux et al., 2013; Sandeep et al., 2014; Seager et al., 2019; Sohn et al., 2013). This difference between observations and climate models could suggest that the climate models’ equatorial Pacific sea surface temperature response to global warming is incorrect, and that projections of associated ENSO teleconnections have limited credibility (C. Michel et al., 2020). As the climate warms, ENSO-driven extreme weather events in Canada, such as droughts, floods, and storms, may become more intense and frequent (e.g., Basu et al., 2020; Del Rio Amador et al., 2023; Sun et al., 2023). These changes could result in more severe impacts on ecosystems and communities.

Figure take-away: The influence of the El Niño–Southern Oscillation on Canadian winter climate variability is expanding eastward as the climate warms.

Figure title: Winter climate anomalies associated with the El Niño–Southern Oscillation in the pre-industrial period and late twenty-first century in Canada

Figure 4.19: Maps of multi-model average anomalies in winter surface air temperature (SAT) in degrees Celsius and precipitation in millimetres per day across Canada associated with the positive phase of the El Niño–Southern Oscillation for the pre-industrial period (1850–1900) (top row) and the late century (2071–2100) (bottom row). The maps are based on 38 CMIP6 model simulations driven by the intermediate emissions scenario (SSP2-4.5). The anomalies are calculated by relating the data to the time series of the Nino 3.4 index and dividing by the standard deviation. Dots indicate anomalies that are statistically significant at the 5% level (meaning there is a ≤ 5% chance of concluding that an effect or trend exists when it does not).
Long description

The figure shows four maps of Canada illustrating how modelled winter surface air temperature (left column) and precipitation (right column) are associated with the positive phase of El Niño for two time periods: the pre industrial era (1850–1900) in the top row and the late twenty-first century (2071–2100) for an intermediate emissions scenario in the bottom row. Regions with black dots overlaid on the shading indicate where anomalies are statistically significant. In the left column, coloured shading shows temperature anomalies in degrees Celsius associated with El Niño. Red indicates warmer than average winters, and blue indicates cooler than average. In both periods, most of Canada warms during El Niño, with warming extending further eastward in the late twenty-century.

In the right column, coloured shading shows precipitation anomalies in millimetres per day. Green indicates wetter than average conditions, and brown indicates drier than average. In both periods, most of Canada dries during El Niño, with drying extending further eastward in the late twenty-first century.

The amplitude of the PDO and associated decade-to-decade variations in temperatures and precipitation are projected to become smaller under global warming (Geng et al., 2019; Lee et al., 2021; L. Zhang & Delworth, 2016). Uncertainties about this weakening arise from uncertainties about the future evolution of the mechanisms that determine the PDO and about how future changes in the average state of the Pacific Ocean will interact with sea surface temperature variability on interannual and decadal timescales (Fedorov et al., 2020). Therefore, there is low confidence in the assessed projected weakening of the PDO. In addition, there is low confidence in the AMO response to climate forcing in the future. Because the AMO operates on multidecadal timescales, the length of climate model projections (which typically end in 2100) may not be sufficient to confidently attribute any changes in the AMO to climate forcings (Lee et al., 2021). Nonetheless, PDO and AMO fluctuations in the coming decades may affect regional climate, including in Canada, compounding or offsetting some of the effects of global warming.

4.8.4: Confidence terms in key messages: summary of evidence

Key message 4.11: The El Niño–Southern Oscillation (ENSO) is the dominant source of year-to-year climate variability in western Canada. Year-to-year climate fluctuations associated with ENSO have been larger since 1950 than in the previous century (medium confidence). However, there is low confidence that this change is due to human-caused climate change because internal climate variability is large.

Key message 4.12: The El Niño–Southern Oscillation (ENSO) will remain the dominant source of climate variability in western Canada in the 21st century (high confidence), but there is low confidence in projected changes in year-to-year climate fluctuations associated with ENSO. While climate models consistently show that by the end of the century, the effect of ENSO on winter climate fluctuations will extend into central and eastern Canada, there is low confidence in these projections due to systematic climate model biases.

We have medium confidence that ENSO amplitude has increased since 1950. This assessment is based on multiple observational and paleoclimate data products. We have low confidence that observed changes in ENSO amplitude and patterns are due to human-caused climate change. This is because climate models show large internal climate variability and a lack of significant trends in ENSO characteristics in recent decades.

We have high confidence that no consistent trends in the PDO and AMO have occurred over the historical period. This assessment is based on multiple observational and paleoclimate data products.

Our high confidence that ENSO will remain the dominant mode of climate variability in the 21st century is due to the strong consensus across all models. We have low confidence that the effect of ENSO on winter climate variability will extend into central and eastern Canada. This is because while climate models consistently project these changes, confidence is limited by persistent model biases. There is some evidence that natural and human-caused external climate forcings have contributed to observed PDO- and AMO-like variability. However, we have low confidence in projections of the PDO and AMO because of complex internal climate variability and inconsistent model representations of these patterns.

4.9: Ocean circulation

Key message 4.13: The primary large-scale ocean current system affecting climate in Canada is the Atlantic Meridional Overturning Circulation (AMOC). A weaker than normal AMOC is associated with cooler and drier than normal winters over eastern Canada. There is high confidence that a temporary weakening of the AMOC between 2007 and 2015 led to a period of cooler North Atlantic Ocean surface temperatures and low confidence that this AMOC weakening can be attributed to human influence.

Key message 4.14: There is high confidence that the Atlantic Meridional Overturning Circulation (AMOC) will gradually weaken over the remainder of the 21st century due to human influence, and that this will slightly reduce the warming of eastern and northern Canada. However, the possibility that the AMOC could shut down, leading to a more pronounced regional cooling influence, cannot be ruled out. There is medium confidence that the AMOC will not shut down in the 21st century.

4.9.1: Effects on Canadian weather and climate

Ocean circulation is driven mainly by winds pushing on the ocean surface, and by flows of heat and freshwater into or out of the ocean that affect the density of seawater. For example, warming by sunlight and freshening due to rainfall tend to make seawater less dense, whereas evaporation enhanced by surface winds tends to make seawater cooler, saltier, and denser. The resulting ocean circulation currents move heat around the globe and play an essential role in shaping the Earth’s climate. Especially important is the oceans’ role in moving heat from tropical regions, where heating by the sun is strongest, toward the Earth’s polar regions. The atmosphere plays a major role in this movement of heat as well. Without this continual movement of heat, temperatures would be even hotter near the equator and colder near the poles.

The Atlantic Meridional Overturning Circulation (AMOC) is vitally important for Northern Hemisphere climate because it transports sinking cold sub-Arctic waters southward and warmer surface waters northward, bringing vast amounts of heat to the North Atlantic. The strength of the AMOC largely determines how much heat it carries, so changes in its strength can strongly affect climate in the North Atlantic. For example, a weaker AMOC exerts a cooling influence that is most pronounced in winter and extends westward from the ocean into eastern Canada. A weaker AMOC also tends to reduce precipitation regionally, resulting in fewer wet winter days in eastern Canada (Bellomo et al., 2023). Variations in the AMOC occur naturally and are a major cause of the Atlantic Multidecadal Oscillation (R. Zhang et al., 2019), whose influence on Canada’s climate is described in section 4.8. Although other ocean current systems vary and may change in a warming climate, none has as large an impact on Canadian weather and climate as the AMOC.

4.9.2: Past changes and their causes

Direct ocean current measurements are too few to provide a clear picture of changes in large-scale currents and associated transports of heat. As a result, such information comes mainly from less direct methods. For example, ocean current velocity can be inferred through its physical relationships with more thoroughly observed ocean properties, such as seawater density and sea level (McCarthy et al., 2020). A notable application of this approach is an array of moored instruments (devices anchored in place to measure ocean properties in one location for an extended period), typically referred to as the RAPID array, which has provided continuous measurements of the strength of the AMOC at a latitude of 26.5°N since 2004 (Kanzow et al., 2008; Srokosz & Bryden, 2015). Additional instrument arrays deployed more recently enable a more complete view of AMOC changes over a shorter period (Lozier, 2023).

Measurements from the RAPID array indicate that the AMOC was relatively strong from 2004 to 2007, became weaker from 2007 to 2015, and regained strength afterward until at least 2020 (Figure 4.20a). These changes were likely caused by the combined influences of changes in winds and the density of seawater (Buckley & Marshall, 2016). During the period when the AMOC was relatively weak, it transported less heat into the North Atlantic than when it was relatively strong (Figure 4.20b) (W. E. Johns et al., 2023). This caused upper ocean temperatures in the subpolar North Atlantic to cool by up to 0.2°C/yr (Figure 4.20c) (Bryden et al., 2020; Jackson et al., 2022), leading to successive years of relatively cold sea surface temperatures in that region. In some years, these cold sea surface temperatures extended to the Newfoundland and Labrador coast (Colbourne et al., 2016). By contrast, upper ocean temperatures in the Gulf of Maine and Scotian Shelf warmed dramatically during the weaker AMOC period (Figure 4.20c). Evidence from observations and model simulations points to the contrasting tendencies in these two regions as being a signature of AMOC variability (R. Zhang et al., 2019). A further tendency that appears to be connected with the weakening of the AMOC is a pronounced drop in oxygen concentrations in Scotian and adjacent shelf waters (Claret et al., 2018), which, along with temperature changes, may affect marine ecosystems in this region (Brennan et al., 2016).

Figure take-away: Recent variations in the Atlantic Meridional Overturning Circulation affect the North Atlantic Ocean.

Figure title: Past variations in the strength of the Atlantic Meridional Overturning Circulation and associated heat transport, and a spatial map of the North Atlantic upper ocean temperature trend from 2007 to 2015

Figure 4.20: Observed variations based on RAPID array measurements of a) Atlantic Meridional Overturning Circulation (AMOC) strength and b) northward transport of heat across 26.5°N in the Atlantic Ocean, where a running one-year average has been applied. AMOC strength is in units of Sverdrups (Sv), where 1 Sv = 1 million m3/s per second, or about 4 to 5 times the flow of the Amazon River; heat transport is in units of Petawatts (PW), where 1 PW = 1015 (million billion) watts, or about 50 times the world’s current total energy production. Values in a) and b) that are larger or smaller than the average for 2004 to 2021 are coloured red and blue respectively. The vertical dashed lines in a) and b) bracket an interval of weaker AMOC strength and heat transport. Shown in c) is the trend of upper ocean temperature (averaged to a depth of 700 m) for 2007 to 2015 when AMOC strength and heat transport were relatively weak, as indicated in a) and b). Dots indicate where the trends are statistically significant at the 5% level (meaning there is a ≤ 5% chance of concluding that an effect or trend exists when it does not), and the horizontal line indicates the latitude of the RAPID array. Adapted from: for a) and b), Johns et al. (2023); for c), Jackson et al. (2022).
Long description

This figure combines two time series panels with a regional ocean temperature trend map to illustrate how variations in the Atlantic Meridional Overturning Circulation (AMOC) affect heat transport and upper ocean temperatures in the North Atlantic. Panels (a) and (b) show annual values from 2004 to 2021 based on RAPID array measurements at 26.5° N. In panel (a), AMOC strength is plotted in Sverdrups, with red shading indicating years when circulation was stronger than the 2004–2021 average and blue shading indicating weaker than average years. Panel (b) presents northward heat transport in petawatts, using the same colour convention. Vertical dashed lines mark a multiyear interval (approximately 2008–2015) when both AMOC strength and heat transport were unusually weak.

Panel (c) maps upper Atlantic Ocean (0–700 m) temperature trends from 2007 to 2015. Blue areas indicate cooling and red areas warming; black dots mark statistically significant trends. The horizontal line shows the location of the RAPID array.

The AMOC’s influences on climate before 2004, when high-quality measurements of AMOC strength and heat transport became available, must be studied using other lines of evidence about which we have less confidence. These lines of evidence include analyses of climate and ocean models, ocean reanalysis datasets (data from ocean models combined with observational data), and observed properties that have a statistical connection with the AMOC, such as sea surface temperature (Jackson et al., 2022). A key observation is that sea surface temperatures in the subpolar North Atlantic have cooled from the late 19th century until the present, even as the rest of the world has warmed. This phenomenon, known as the North Atlantic warming hole, is also present in climate models’ historical simulations. One potential explanation is that this regional cooling trend could be linked to a human-caused weakening of the AMOC (K.-Y. Li & Liu, 2025). Such a weakening has been inferred from patterns of sea surface temperature change and other indirect lines of evidence (Caesar et al., 2018, 2021; Rahmstorf et al., 2015). However, climate scientists have debated whether the evidence for these inferred changes is robust (Kilbourne et al., 2022; S. L. L. Michel et al., 2025; Terhaar et al., 2025; Worthington et al., 2021) and whether the changes are caused by internal climate variability rather than human activity (Latif et al., 2022). In addition, CMIP6 historical climate simulations show no clear long-term decrease in the AMOC (blue curve and shading in Figure 4.21a) (Fox-Kemper et al., 2021; Jackson et al., 2022). Instead, these simulations show AMOC strength gradually increasing on average from 1850 until the late 20th century. This strengthening in the CMIP6 models is caused by the simulated influences of human-caused aerosols on clouds, although observational evidence suggests that CMIP6 models may overestimate this influence (Menary et al., 2020). While these simulations show AMOC strength decreasing on average from the late 20th century until the present due to the increasing atmospheric greenhouse gas concentrations, these changes are relatively small and gradual compared to the observed shorter-term variations (black curve in Figure 4.21a), which evidently are dominated by internal climate variability (Eyring et al., 2021a, Section 3.5.4.1).

Overall, there is high confidence that between 2004 and the present, the AMOC weakened and then partially recovered, and low confidence that these changes were forced by human factors. In addition, there is low confidence that AMOC strength has been influenced by human activity since the late 19th century. This is not inconsistent with the existence of the North Atlantic warming hole because other processes that may have contributed to its formation have been identified. These processes include increased poleward heat transport out of the subpolar North Atlantic region, with some contribution from increased low-level clouds (Keil et al., 2020), and increased cooling of the ocean surface caused by changes in winds (Fan et al., 2023; He et al., 2022; Hu & Fedorov, 2020; L. Li et al., 2022).

Figure take-away: Past and future changes in the Atlantic Meridional Overturning Circulation have implications for climate in Canada.

Figure title: Time series of observed and simulated past and future Atlantic Meridional Overturning Circulation strength, and the effect of its future weakening on annual average Canadian temperatures

Figure 4.21: Past and future changes in the Atlantic Meridional Overturning Circulation and their implications for climate in Canada. a) Simulated changes in running 10-year averages of Atlantic Meridional Overturning Circulation (AMOC) strength in CMIP6 historical simulations (blue) and under a very high emissions scenario (red; SSP5-8.5). The blue and red lines represent averages over the many simulations considered, and the corresponding shadings indicate ranges containing approximately 95% of the simulated values. The horizontal dashed lines indicate this range in simulations representing conditions in 1850, whereas observed yearly averages of AMOC strength from the RAPID array are indicated in black. Adapted from: Jackson et al. (2022). b) Change (warming) between temperatures averaged over 1961 to 1980 and 2061 to 2080 under a very high emissions scenario. c) Reduction in this warming caused by AMOC weakening, as determined by comparing to a simulation in which AMOC strength is artificially held steady. Dots in b) and c) indicate that the change is statistically significant at the 5% level (meaning there is a ≤ 5% chance of concluding that an effect or trend exists when it does not). Adapted from: W. Liu et al. (2020).
Long description

This figure shows how changes in the Atlantic Meridional Overturning Circulation (AMOC)—a major system of ocean currents that transports heat northward—affect climate in Canada. Panel (a) is a time series of AMOC anomalies from 1850 to 2100. A black line shows observed AMOC strength, while the blue and red shaded regions show modelled historical and future AMOC values under a high emissions scenario. The shaded envelopes represent the range of results across many climate models. Observations and simulations indicate relatively stable AMOC strength in the historical period, followed by a pronounced weakening through the 21st century.

Panels (b) and (c) show maps of projected annual mean temperature change between 1961–1980 and 2061–2080. Panel (b) shows warming expected with a weakening AMOC, while panel (c) isolates the reduction in warming due specifically to AMOC weakening. Areas with black dots mark changes that are statistically robust. Results indicate that AMOC weakening slightly reduces warming in eastern Canada, although strong warming still dominates across the country.

4.9.3: Future changes

Although it is uncertain whether human-caused warming has resulted in an AMOC weakening between the late 19th and early 21st centuries, there is high confidence in climate model projections of a weakening AMOC over the remainder of the 21st century in response to greenhouse gas emissions from human activity (red curve and shading in Figure 4.21a) (Jackson et al., 2022). This weakening is projected under all CMIP6 emissions scenarios, ranging from very low to very high emissions (Fox-Kemper et al., 2021; Weijer et al., 2020). The magnitude of the weakening does not heavily depend on the emissions scenario (e.g., Bonan et al., 2025). However, there is low confidence in how much weakening will occur by 2100, due mainly to differences between models in simulating projected responses of the AMOC, although ways to reduce this uncertainty have been explored (Bonan et al., 2025). A major cause of the simulated weakening is increased input of heat and freshwater into the subpolar North Atlantic (e.g., Madan et al., 2024). This increase in heat and freshwater reduces the density of surface waters and inhibits the sinking motions that help drive the AMOC. Climate model experiments indicate that melting of Arctic sea ice (W. Liu et al., 2019), which is fresher than seawater, and meltwater from the Greenland ice sheet (Bakker et al., 2016) will contribute to this process.

Climate model projections consistently show a relative lack of warming of surface air temperature across a subpolar North Atlantic region (Figure 4.21b) (Fox-Kemper et al., 2021; W. Liu et al., 2020) similar to that of the observed North Atlantic warming hole (Keil et al., 2020). In contrast to the uncertain contribution of AMOC weakening to the long-term past cooling in this region, AMOC weakening is a primary cause of this projected lack of warming (Menary & Wood, 2018). Climate model experiments have explored the extent to which the projected AMOC weakening may reduce the amount of warming in different regions. For example, one experiment compared a very high emissions scenario (SSP5-8.5) simulation, with strong AMOC weakening, to one in which AMOC strength was artificially held steady (W. Liu et al., 2020). The experiment found that AMOC weakening reduced warming across the subpolar North Atlantic and Labrador Sea from 1961 to 1980 and from 2061 to 2080 by up to 3°C (Figure 4.21c). Warming across eastern and northern Canada was similarly reduced by about 1°C because of the projected weakening of the AMOC. However, this cooling effect only partially offsets the projected warming of over 3°C across Canada under this scenario in this climate model (Figure 4.21b). In this example, the AMOC weakened by about 25% over the interval considered, but in other simulations the AMOC weakens more or less depending on the model and scenario (Lee et al., 2021). Therefore, while the results in Figure 4.21 b) and c) illustrate the probable effects of AMOC weakening on surface warming, the magnitude and timing of these effects is uncertain (Fox-Kemper et al., 2021).

Additional climate model experiments have explored what will happen to the AMOC if global warming is limited to 1.5°C or 2.0°C. In these experiments, the AMOC continues to decline for a few years after global temperatures stabilize, but then gradually recovers to nearly pre-warming levels after about 150 years (Lee et al., 2021; Sigmond et al., 2020). Because a stronger AMOC carries more heat to the North Atlantic, this region warms during the period of AMOC recovery despite global temperatures having stabilized. The future North Atlantic warming hole caused by the previous weakening of the AMOC (Figure 4.21b) is effectively “filled in.” A similar sequence of events occurs if global temperatures rise to 3.0°C above pre-industrial levels before stabilizing.

A further possibility that has been explored is whether the projected changes in the subpolar North Atlantic, especially increased inputs of freshwater, could cause the AMOC to abruptly shut down (Weijer et al., 2019). This is motivated by studies of climate and ocean circulation in the last Ice Age, showing that the AMOC abruptly weakened or shut down numerous times between about 80,000 and 11,700 years ago (Lynch-Stieglitz, 2017). Those episodes are believed to have been caused by sudden large inputs of buoyant freshwater from ice sheet melt or discharge, shutting off the sinking of dense subpolar North Atlantic surface waters that helps drive the AMOC. Their effects on climate included rapid cooling of the Northern Hemisphere, especially in the North Atlantic region. This has prompted climate model experiments that artificially impose an unrealistically large freshening of the North Atlantic to induce an AMOC shutdown (Jackson et al., 2023). Such experiments indicate that the cooling effect of an AMOC shutdown would far exceed that of the projected AMOC weakening illustrated in Figure 4.21 c) (Jackson et al., 2023; W. Liu et al., 2017; Weijer et al., 2019).

Whether the AMOC could actually shut down during the 21st century or beyond is a separate question. Climate model projections do not simulate a 21st century AMOC shutdown even under very high emissions scenarios (Fox-Kemper et al., 2021). However, they do not represent some processes that may increase meltwater release from the Greenland ice sheet, such as accelerated flow of ice into the ocean. Nonetheless, estimates of future Greenland meltwater release from a detailed ice sheet model, while tending to weaken the AMOC, are still insufficient to trigger a 21st century shutdown (Golledge et al., 2019). Some scientists have argued that the AMOC in climate models is unrealistically stable because of systematic model errors, and that simulated AMOC shutdown can occur when these errors are corrected (W. Liu et al., 2017). Additional studies have cited modelling and observational evidence to assert that an AMOC shutdown could be much more likely than standard climate simulations indicate (Ditlevsen & Ditlevsen, 2023; van Westen et al., 2024). However, further work is needed before a scientific consensus can be reached on this question, and currently there is medium confidence that the AMOC will not shut down in the 21st century (J. A. Baker et al., 2025; Fox-Kemper et al., 2021).

Changes in ocean current systems besides the AMOC are less likely to directly impact climate in Canada. There is, however, evidence from climate model experiments that warming-induced changes in wind-driven ocean circulation act as a positive feedback that modestly amplifies the rate of warming, including over central and eastern Canada (McMonigal et al., 2023).

4.9.4: Confidence terms in key messages: summary of evidence

Key message 4.13: The primary large-scale ocean current system affecting climate in Canada is the Atlantic Meridional Overturning Circulation (AMOC). A weaker than normal AMOC is associated with cooler and drier than normal winters over eastern Canada. There is high confidence that a temporary weakening of the AMOC between 2007 and 2015 led to a period of cooler North Atlantic Ocean surface temperatures and low confidence that this AMOC weakening can be attributed to human influence.

Key message 4.14: There is high confidence that the Atlantic Meridional Overturning Circulation (AMOC) will gradually weaken over the remainder of the 21st century due to human influence, and that this will slightly reduce the warming of eastern and northern Canada. However, the possibility that the AMOC could shut down, leading to a more pronounced regional cooling influence, cannot be ruled out. There is medium confidence that the AMOC will not shut down in the 21st century.

We have high confidence that a temporary weakening of the AMOC led to a cooling of North Atlantic Ocean surface temperatures from 2007 to 2015. This assessment is based on the availability of reliable AMOC observations since 2004 and the consistency between the observed AMOC heat transport changes and North Atlantic Ocean temperature trends. However, because of large internal climate variability and the short observational period, we have low confidence that these changes were anthropogenically forced.

We have high confidence that subpolar North Atlantic surface temperatures have cooled since the late 19th century, based on high consistency between different reanalysis datasets. However, we have low confidence that this was caused by an anthropogenically forced weakening of the AMOC, because historical simulations with climate models do not consistently show a long-term decline in the AMOC.

Owing to high consistency among climate model projections and across scenarios, we have high confidence that the AMOC will weaken over the 21st century due to human influence, and that this will reduce the rate of warming in the subpolar North Atlantic and nearby regions, including eastern and northern Canada. While the projected magnitude of AMOC reductions is not very sensitive to emissions scenario, we have low confidence in the magnitude of the AMOC reductions and corresponding consequences for regional climate, due to a large model spread.

While climate models do not project a shutdown of the AMOC in the 21st century, there is only medium confidence in these projections. This is because the AMOC in climate models may be more stable than in reality, as the models do not represent all the processes that affect the AMOC. Therefore, a shutdown of the AMOC in the 21st century cannot be ruled out.

4.10: Synthesis of changes in atmosphere-ocean processes and phenomena

Key message 4.15: Changes that are due to thermodynamic processes are generally robust and well understood.

Key message 4.16: Regional variations in Canadian climate depend strongly on changes in dynamical processes, which are uncertain and less well understood.

Key message 4.17: There is generally more confidence in future human-caused changes than in the attribution of past changes to human-caused climate change.

Compared to CCCR2019, this chapter has been added to assess large-scale atmosphere-ocean processes and phenomena that are relevant to past and future regional variations in Canadian climate. The assessment of these processes and phenomena strengthens the basis of our understanding of other aspects of climate change in Canada assessed in other chapters. This synthesis provides a high-level overview of our main conclusions on large-scale atmosphere-ocean processes and phenomena.

Key Message 4.15 states that changes that are due to thermodynamic processes are generally robust and well understood. This is because changes in thermodynamic processes are directly caused by changes in the radiative balance as a result of human-caused increases in greenhouse gas concentrations. At high latitudes, such changes are amplified through local climate processes, leading to a phenomenon referred to as Arctic amplification. This phenomenon largely explains why northern Canada warms faster than other parts of Canada. Human-caused global warming also results in an increased availability of moisture in the atmosphere, which acts to amplify precipitation across Canada, including that associated with atmospheric rivers and North Atlantic hurricanes. There is evidence that thunderstorm activity across Canada will increase as well, but such changes are less certain because of limitations in the climate models that underpin these projections.

Key Message 4.16 states that regional variations in Canadian climate depend strongly on changes in dynamical processes, which are uncertain and less well understood. Changes in the atmospheric circulation, such as the strength and position of the jet stream, extratropical storms, and atmospheric blocks, are critical to understanding regional patterns of climate change in Canada but are less certain than changes associated with thermodynamic processes. This is because of:

  1. the large role of internal climate variability, which is inherently unpredictable beyond a few years
  2. the fact that changes in atmospheric circulation are generally driven by gradients (or spatial differences) in temperature changes
    1. Note: Under climate change, different processes lead to opposing changes in large-scale temperature gradients, resulting in relatively small net changes in the atmospheric circulation.
  3. limitations of climate models
    1. Note: A notable example is that while climate models consistently project that year-to-year climate variability associated with the El Niño–Southern Oscillation will increase across Canada, there is a large degree of uncertainty due to systematic climate model biases in the tropical Pacific, the key region of the El Niño–Southern Oscillation.  

Key Message 4.17 states that there is generally more confidence in future human-caused changes than in the attribution of past changes to human-caused climate change. This statement is true for several processes assessed in this chapter, including atmospheric rivers, rain rates associated with North Atlantic hurricanes affecting Canada, large-scale environmental conditions favouring thunderstorms, and changes in the Atlantic Meridional Overturning Circulation. This is because:

  1. past climate changes are often heavily influenced by internal climate variability, making it challenging to determine if such changes are due to human-caused climate change;
  2. past climate changes are relatively small compared to future climate changes, at least in intermediate (SSP2-4.5) to high (SSP3-7.0) emissions scenarios; and
  3. many observational datasets are relatively short.

4.11: Knowledge gaps

Much of the uncertainty in projections of regional variations in Canadian climate is due to internal climate variability, which is inherently unpredictable beyond a few years, and hence cannot be reduced. However, the following knowledge gaps can be narrowed with future efforts.

Understanding mechanisms responsible for changes in the atmospheric circulation and their representation in climate models

While changes in the atmospheric circulation are thought to be driven by changes in large-scale spatial differences in temperature changes, the underlying mechanisms are poorly understood. For example, a theoretical framework on how atmospheric blocks respond to global warming is lacking. Progress can be made by conducting systematic studies using idealized experiments with a hierarchy of models of different complexity (P. Maher et al., 2019) and by leveraging other existing and emerging tools (T. A. Shaw et al., 2024).

There is also uncertainty about how well these processes are captured in current climate models. While climate models tend to project a poleward shift of the jet streams in response to climate change, some studies have questioned the reliability of such projections. In particular, it has been suggested that climate models systematically underestimate the response to Arctic climate change (Screen et al., 2022; Smith et al., 2022), and that after correction of this underestimation, there would be a net projected equatorward shift, not the poleward shift of the uncorrected projections (Screen et al., 2022). However, new evidence suggests that climate models do not systematically underestimate the jet stream response to Arctic climate change (Sigmond & Sun, 2025), highlighting the need for further studies. In addition, climate models are not able to simulate the amplitude of past changes in the North Pacific jet stream (Patterson & O’Reilly, 2025) and North Atlantic jet stream (Blackport & Fyfe, 2022), which calls into question the reliability of projections. Resolving these model-observation discrepancies should therefore be a high research priority.

Attributing past long-term trends in atmospheric-river activity

While observations show that the frequency and intensity of atmospheric rivers have increased over Canada in recent decades, there are currently no studies that have tried to attribute such changes to human activity. There is evidence that recent extreme atmospheric-river events have been made more likely by climate change, but attribution studies on the long-term trends are currently lacking.

More studies focused on the impacts of North Atlantic hurricanes in Canada

While it is well established that the intensity of North Atlantic hurricanes will increase in the future as a result of human-caused climate change, studies on hurricanes that affect Canada are sparse. Given the potentially large impacts these changes have on extreme rain and wind events in eastern Canada, studies focused on Canada would improve understanding of this topic.  

Reducing tropical Pacific climate model biases to increase confidence in the impacts of the El Niño–Southern Oscillation (ENSO) on Canada

Climate models consistently show that future human-caused climate change will act to extend ENSO-related year-to-year climate variability into eastern Canada. While such a high level of model agreement typically leads to confident projections, there is a concern that there is a common bias in climate models that may lead to incorrect projections. Specifically, there is persistent cooling of the eastern equatorial Pacific in observations over recent decades, which cannot be reproduced by current climate models. Resolving this discrepancy through climate model improvements would lead to a better understanding and to more confident projections of the impact of ENSO on Canadian climate variability.  

Representation of the Atlantic Meridional Overturning Circulation (AMOC) in climate models

Climate models consistently project that the AMOC will weaken in response to human-caused climate warming. However, there is much uncertainty about the magnitude of this weakening, with some studies arguing that the AMOC could even shut down during the 21st century. While current climate models do not project such a shutdown, these claims are based on the fact that climate models do not properly represent the impacts of the melting of the Greenland Ice Sheet, and some evidence that suggests that the AMOC in climate models is unrealistically stable because of other systematic model errors. Resolving these issues will increase confidence in projections of winter climate in eastern Canada.

FAQs

FAQ 4.1: Why is Canada warming faster than the world as a whole?

The Earth’s climate is heating up because of increasing greenhouse gas emissions from human activity, primarily the burning of fossil fuels (Chapter 1, section 1.1). The response of global surface temperature to increasing greenhouse gas emissions is not spatially uniform. Greater warming of the surface over land than over oceans is observed because the oceans’ greater heat capacity slows down warming over oceans relative to warming over land. Greater warming in the Arctic than for the world as a whole is also observed because climate feedbacks amplify warming in this region, a phenomenon known as Arctic amplification. Both of these factors contribute to the fact that Canada, and the Canadian Arctic in particular, is warming at a faster rate than the global average.

Figure take-away: Canada has warmed at nearly twice the rate of the global average, and Canada’s Arctic has warmed at three times the rate of the global average since 1970.

Figure title: Surface temperature trends for Canada, the Canadian Arctic, and the global average

FAQ 4.1 Figure 1: Observations of annual average surface temperature for the Canadian Arctic (magenta curve), for Canada (blue curve), the global land area (green curve), and the combined global land and ocean area (gray curve) from 1950 to 2023. Data consist of the average of four surface temperature data products: three observationally based gridded products, GISTEMP, HadCRUT5, and Berkeley Earth, and one reanalysis product, ERA5. Lines of best fit are for the time period from 1970 to 2023. Anomalies are relative to a reference period of 1961 to 1990. The Canadian Arctic is bounded by 66.5°N to 83.11°N and 219°E to 307.38°E. Data source: three observationally based gridded products, GISTEMP (Lenssen et al., 2019b), HadCRUT5 (Morice et al., 2021), and Berkeley Earth (Rohde & Hausfather, 2020), and one reanalysis product, ERA5 (Hersbach et al., 2020).
Long description

The figure shows four time series of surface temperature anomalies (relative to the 1961–1990 mean) for four different regions: the Canadian Arctic (magenta line), Canada (blue line) the global land area (green line), and the combined global land and ocean area (grey line). The horizontal axis spans the years 1950 to 2023 and the vertical axis ranges from -2 to 4 °C. Linear trend lines are plotted for each time series for the 1970–2023 period only. The slopes of these four trend lines are all positive, indicating warming, and show that the rate of surface warming for Canada is nearly twice the global rate, while the rate of warming for the Canadian Arctic is three times the global rate for the 1970–2023 period.

FAQ 4.1 Figure 1 shows that Canada’s rate of surface warming has been close to two times the global rate for the period 1970-2023. This is partly because Canada is mostly land and also because of the phenomenon of Arctic amplification. Given the smaller heat capacity of land, land areas warm more quickly than ocean areas. This is evident in the figure, which shows that for 1970-2023 the global land area has warmed about 50% faster than the combined global surface temperature, which combines surface air temperature over land and sea surface temperatures. Furthermore, Canada’s location at mid-to-high latitudes means that warming in Canada is amplified by local climate feedbacks. In the Canadian Arctic, Arctic amplification contributes to an even greater rate of warming, about three times the global rate for the period 1970-2023 (learn more about Arctic amplification in section 4.2 and Box 4.2). Note that the warming rates shown in FAQ 4.1 Figure 1 are based on the average of four gridded global surface temperature data products. These products are used for consistency across the global and Canadian regions. In Chapter 2, data products specific to Canada (see gridded station data in section 2.3.4.1 for details) are used to assess past surface temperature change in Canada and show similar warming rates (section 2.4.1). Source: Chapter 4, section 4.2.

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Supplementary Material

Figure take-away: The positive NAO phase is associated with a stronger jet stream and colder and drier conditions over eastern Canada.

Figure title: The winter wind, temperature, and precipitation patterns associated with the positive phase of the North Atlantic Oscillation

Supplementary Figure S4.1: Maps showing winter climate patterns in Canada associated with the positive phase of the North Atlantic Oscillation. The winter a) west-to-east wind speed at 700 hPa (about 3 km above the Earth’s surface), b) temperature, and c) precipitation anomalies (relative to average conditions) associated with a positive North Atlantic Oscillation (NAO). The anomalies are calculated by relating the historical data for Canada to the time series of the NAO index for the period from 1951 to 2023. The NAO index was calculated by first taking the difference in area average sea level pressure between the Azores (20–28°W, 36–40°N) and Iceland (16–25°W, 63–70°N) and then dividing it by the standard deviation. The linear trend was removed from all data prior to the calculations. The dots indicate where the trends are statistically significant after controlling for the false discovery rate at the 10% significance level (meaning there is a ≤ 10% chance of concluding that an effect or trend exists when it does not). Data source: ERA5 reanalysis.
Long description

These three maps show how winter climate conditions in Canada typically change during the positive phase of the North Atlantic Oscillation (NAO), when the jet stream is stronger and located more northward than average. Panel a displays anomalies in west to east wind speed at about 3 km altitude (700 hPa). The figure shows a broad band of stronger than normal westerly winds stretching across eastern Canada and the northwest Atlantic, indicating an intensified jet stream. Areas with significant changes are marked with black dots. Panel b shows temperature anomalies, with widespread cooler than average conditions across eastern and central Canada, particularly over Quebec and Labrador, and pockets of slight warming farther south. Panel c depicts precipitation anomalies. Eastern Canada generally becomes drier than normal. All anomalies are calculated by relating 1951–2023 historical climate data to the NAO index. Data originate from the ERA5 reanalysis.

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2026-09-03