Frozen water is found on the
Earth’s surface primarily as
snow cover,
freshwater ice in
lakesand
rivers,
sea ice,
glaciers,
ice sheets, and frozen ground and
permafrost (permanently frozen ground). The residence time of water in each of these cryospheric sub-systems varies widely. Snow cover and freshwater ice are essentially seasonal, and most sea ice, except for ice in the central
Arctic, lasts only a few years if it is not seasonal. A given water particle in
glaciers,
ice sheets, or ground ice, however, may remain frozen for 10–100,000 years or longer, and deep ice in parts of
East Antarctica may have an age approaching 1 million years.
Most of the world's ice volume is in
Antarctica, principally in the
East Antarctic Ice Sheet. In terms of areal extent, however,
Northern Hemisphere winter snow and ice extent comprise the largest area, amounting to an average 23% of hemispheric surface area in January. The large areal extent and the important climatic roles of
snow and
ice, related to their unique physical properties, indicate that the ability to observe and model snow and ice-cover extent, thickness, and
physical properties (radiative and thermal properties) is of particular significance for
climate research.
There are several fundamental physical properties of snow and ice that modulate energy exchanges between the surface and the
atmosphere. The most important properties are the surface reflectance (
albedo), the ability to transfer heat (thermal diffusivity), and the ability to change state (
latent heat). These physical properties, together with surface roughness,
emissivity, and
dielectric characteristics, have important implications for observing
snow and
ice from space. For example, surface roughness is often the dominant factor determining the strength of
radar backscatter .
[2] Physical properties such as
crystal structure, density, length, and liquid water content are important factors affecting the transfers of heat and water and the scattering of
microwave energy.
The surface reflectance of incoming
solar radiation is important for the surface energy balance (SEB). It is the ratio of reflected to incident solar radiation, commonly referred to as
albedo.
Climatologists are primarily interested in
albedo integrated over the
shortwave portion of the
electromagnetic spectrum (~300 to 3500 nm), which coincides with the main solar energy input. Typically,
albedo values for non-melting snow-covered surfaces are high (~80–90%) except in the case of forests. The higher
albedos for snow and ice cause rapid shifts in surface
reflectivity in autumn and spring in high latitudes, but the overall climatic significance of this increase is spatially and temporally modulated by
cloud cover. (Planetary
albedo is determined principally by
cloud cover, and by the small amount of total
solar radiation received in high
latitudes during winter months.) Summer and autumn are times of high-average cloudiness over the
Arctic Ocean so the
albedo feedbackassociated with the large seasonal changes in
sea-ice extent is greatly reduced. Groisman
et al.[3] observed that snow cover exhibited the greatest influence on the
Earth radiative balance in the spring (April to May) period when incoming
solar radiation was greatest over snow-covered areas.
[3]
The
thermal properties of cryospheric elements also have important climatic consequences.
Snow and
ice have much lower
thermaldiffusivities than
air.
Thermal diffusivity is a measure of the speed at which temperature waves can penetrate a substance.
Snow and
ice are many
orders of magnitude less efficient at diffusing heat than
air. Snow cover insulates the ground surface, and sea ice insulates the underlying ocean, decoupling the surface-atmosphere interface with respect to both heat and moisture fluxes. The flux of moisture from a water surface is eliminated by even a thin skin of ice, whereas the flux of heat through thin ice continues to be substantial until it attains a thickness in excess of 30 to 40 cm. However, even a small amount of snow on top of the ice will dramatically reduce the heat flux and slow down the rate of ice growth. The insulating effect of snow also has major implications for the
hydrological cycle. In non-permafrost regions, the insulating effect of snow is such that only near-surface ground freezes and deep-water drainage is uninterrupted.
[4]
While
snow and
ice act to insulate the surface from large energy losses in winter, they also act to retard warming in the spring and summer because of the large amount of energy required to melt ice (the
latent heat of fusion, 3.34 x 10
5 J/kg at 0 °C). However, the strong static stability of the
atmosphere over areas of extensive snow or ice tends to confine the immediate cooling effect to a relatively shallow layer, so that associated atmospheric anomalies are usually short-lived and local to regional in scale.
[5] In some areas of the world such as
Eurasia, however, the cooling associated with a heavy snowpack and moist spring soils is known to play a role in modulating the summer
monsooncirculation.
[6] Gutzler and Preston (1997) recently presented evidence for a similar snow-summer circulation
feedback over the southwestern
United States.
[7]
The role of
snow cover in modulating the monsoon is just one example of a short-term cryosphere-climate
feedback involving the land surface and the
atmosphere. From Figure 1 it can be seen that there are numerous cryosphere-climate feedbacks in the
global climatesystem. These operate over a wide range of spatial and temporal scales from local seasonal cooling of air temperatures to hemispheric-scale variations in
ice sheets over time-scales of thousands of years. The
feedback mechanisms involved are often complex and incompletely understood. For example, Curry
et al. (1995) showed that the so-called “simple” sea ice-albedo feedback involved complex interactions with lead fraction, melt ponds, ice thickness, snow cover, and sea-ice extent.
Snow cover has the second-largest areal extent of any component of the cryosphere, with a mean maximum areal extent of approximately 47 million km
2. Most of the Earth's snow-covered area (SCA) is located in the
Northern Hemisphere, and
temporal variability is dominated by the seasonal cycle;
Northern Hemisphere snow-cover extent ranges from 46.5 million km
2 in January to 3.8 million km
2 in August.
[8] North American winter SCA has exhibited an increasing trend over much of this century
[9][10] largely in response to an increase in precipitation.
[11]However, the available
satellite data show that the hemispheric winter snow cover has exhibited little interannual variability over the 1972–1996 period, with a coefficient of variation (COV=s.d./mean) for January
Northern Hemisphere snow cover of < 0.04. According to Groisman
et al.[3] Northern Hemisphere spring snow cover should exhibit a decreasing trend to explain an observed increase in
Northern Hemispherespring
air temperatures this century. Preliminary estimates of SCA from historical and reconstructed
in situ snow-cover data suggest this is the case for
Eurasia, but not for
North America, where spring snow cover has remained close to current levels over most of this century.
[12]Because of the close relationship observed between hemispheric air temperature and snow-cover extent over the period of
satellite data (IPCC 1996), there is considerable interest in monitoring
Northern Hemisphere snow-cover extent for detecting and monitoring
climate change.
Snow cover is an extremely important storage component in the water balance, especially seasonal
snowpacks in mountainous areas of the world. Though limited in extent, seasonal
snowpacks in the
Earth’s mountain ranges account for the major source of the runoff for stream flow and
groundwater recharge over wide areas of the midlatitudes. For example, over 85% of the annual runoff from the
Colorado Riverbasin originates as snowmelt.
Snowmelt runoff from the Earth's mountains fills the rivers and recharges the aquifers that over a billion people depend on for their water resources. Furthermore, over 40% of the world's protected areas are in mountains, attesting to their value both as unique
ecosystems needing protection and as recreation areas for humans. Climate warming is expected to result in major changes to the partitioning of snow and rainfall, and to the timing of snowmelt, which will have important implications for water use and management. These changes also involve potentially important decadal and longer time-scale
feedbacks to the climate system through temporal and spatial changes in
soil moisture and runoff to the
oceans.(Walsh 1995). Freshwater fluxes from the snow cover into the marine environment may be important, as the total flux is probably of the same magnitude as desalinated ridging and rubble areas of sea ice.
[13] In addition, there is an associated pulse of precipitated pollutants which accumulate over the Arctic winter in snowfall and are released into the ocean upon
ablation of the
sea-ice .
Sea ice covers much of the polar oceans and forms by freezing of sea water.
Satellite data since the early 1970s reveal considerable seasonal, regional, and interannual variability in the
sea-ice covers of both hemispheres. Seasonally, sea-ice extent in the
Southern Hemisphere varies by a factor of 5, from a minimum of 3–4 million km
2 in February to a maximum of 17–20 million km
2 in September.
[14][15] The seasonal variation is much less in the Northern Hemisphere where the confined nature and high latitudes of the
Arctic Ocean result in a much larger perennial ice cover, and the surrounding land limits the equatorward extent of wintertime ice. Thus, the seasonal variability in
Northern Hemisphere ice extent varies by only a factor of 2, from a minimum of 7–9 million km
2 in September to a maximum of 14–16 million km
2 in March.
[15][16]
The ice cover exhibits much greater regional-scale interannual variability than it does hemispherical. For instance, in the region of the
Sea of Okhotsk and
Japan, maximum ice extent decreased from 1.3 million km
2 in 1983 to 0.85 million km
2 in 1984, a decrease of 35%, before rebounding the following year to 1.2 million km
2.
[15] The regional fluctuations in both hemispheres are such that for any several-year period of the
satellite record some regions exhibit decreasing ice coverage while others exhibit increasing ice cover.
[17] The overall trend indicated in the passive microwave record from 1978 through mid-1995 shows that the extent of
Arctic sea ice is decreasing 2.7% per decade.
[18]Subsequent work with the satellite passive-microwave data indicates that from late October 1978 through the end of 1996 the extent of
Arctic sea ice decreased by 2.9% per decade while the extent of
Antarctic sea ice increased by 1.3% per decade.
[19] The Intergovernmental Panel on Climate Change publication
Climate change 2013: The Physical Science Basis stated that sea ice extent for the
Northern Hemisphereshowed a decrease of 3.8% ± 0.3% per decade from November 1978 to December 2012.
[20]
Lake ice and river iceEdit
Ice forms on
rivers and
lakes in response to seasonal cooling. The sizes of the ice bodies involved are too small to exert anything other than localized climatic effects. However, the freeze-up/break-up processes respond to large-scale and local weather factors, such that considerable interannual variability exists in the dates of appearance and disappearance of the ice. Long series of lake-ice observations can serve as a proxy climate record, and the monitoring of freeze-up and break-up trends may provide a convenient integrated and seasonally-specific index of climatic perturbations. Information on river-ice conditions is less useful as a climatic proxy because ice formation is strongly dependent on river-flow regime, which is affected by precipitation, snow melt, and watershed runoff as well as being subject to human interference that directly modifies channel flow, or that indirectly affects the runoff via land-use practices.
Lake freeze-up depends on the heat storage in the lake and therefore on its depth, the rate and temperature of any
inflow, and water-air energy fluxes. Information on lake depth is often unavailable, although some indication of the depth of shallow lakes in the
Arctic can be obtained from airborne
radar imagery during late winter (Sellman
et al. 1975) and spaceborne optical imagery during summer (Duguay and Lafleur 1997). The timing of breakup is modified by snow depth on the ice as well as by ice thickness and freshwater inflow.
Frozen ground and permafrostEdit
Frozen ground (permafrost and seasonally frozen ground) occupies approximately 54 million km
2 of the exposed land areas of the Northern Hemisphere (Zhang et al., 2003) and therefore has the largest areal extent of any component of the cryosphere.
Permafrost (perennially frozen ground) may occur where mean annual air temperatures (MAAT) are less than −1 or −2 °C and is generally continuous where MAAT are less than −7 °C. In addition, its extent and thickness are affected by ground moisture content,
vegetation cover, winter snow depth, and aspect. The global extent of permafrost is still not completely known, but it underlies approximately 20% of
Northern Hemisphere land areas. Thicknesses exceed 600 m along the Arctic coast of northeastern Siberia and Alaska, but, toward the margins, permafrost becomes thinner and horizontally discontinuous. The marginal zones will be more immediately subject to any melting caused by a warming trend. Most of the presently existing permafrost formed during previous colder conditions and is therefore relic. However, permafrost may form under present-day polar climates where glaciers retreat or land emergence exposes unfrozen ground. Washburn (1973) concluded that most continuous permafrost is in balance with the present climate at its upper surface, but changes at the base depend on the present climate and geothermal heat flow; in contrast, most discontinuous permafrost is probably unstable or "in such delicate equilibrium that the slightest climatic or surface change will have drastic disequilibrium effects".
[21]
Under warming conditions, the increasing depth of the summer
active layer has significant impacts on the
hydrologic and
geomorphicregimes. Thawing and retreat of
permafrost have been reported in the upper
Mackenzie Valley and along the southern margin of its occurrence in
Manitoba, but such observations are not readily quantified and generalized. Based on average latitudinal gradients of air temperature, an average northward displacement of the southern
permafrost boundary by 50-to-150 km could be expected, under equilibrium conditions, for a 1 °C warming.
Only a fraction of the permafrost zone consists of actual ground ice. The remainder (dry permafrost) is simply soil or rock at subfreezing temperatures. The ice volume is generally greatest in the uppermost permafrost layers and mainly comprises pore and segregated ice in
Earth material. Measurements of bore-hole temperatures in permafrost can be used as indicators of net changes in temperature regime. Gold and Lachenbruch (1973) infer a 2–4 °C warming over 75 to 100 years at
Cape Thompson,
Alaska, where the upper 25% of the 400-m thick
permafrost is unstable with respect to an equilibrium profile of temperature with depth (for the present mean annual surface temperature of −5 °C).
Maritime influences may have biased this estimate, however. At
Prudhoe Bay similar data imply a 1.8 °C warming over the last 100 years (Lachenbruch
et al. 1982). Further complications may be introduced by changes in snow-cover depths and the natural or artificial disturbance of the surface vegetation.
The potential rates of permafrost thawing have been established by Osterkamp (1984) to be two centuries or less for 25-meter-thick permafrost in the discontinuous zone of interior
Alaska, assuming warming from −0.4 to 0 °C in 3–4 years, followed by a further 2.6 °C rise. Although the response of permafrost (depth) to temperature change is typically a very slow process (Osterkamp 1984; Koster 1993), there is ample evidence for the fact that the
active layer thickness quickly responds to a temperature change (Kane
et al. 1991). Whether, under a warming or cooling scenario, global climate change will have a significant effect on the duration of frost-free periods in both regions with seasonally and perennially frozen ground.
Glaciers and ice sheetsEdit
Ice sheets and
glaciers are flowing ice masses that rest on solid land. They are controlled by snow accumulation, surface and basal melt, calving into surrounding oceans or lakes and internal dynamics. The latter results from gravity-driven creep flow ("
glacial flow") within the ice body and sliding on the underlying land, which leads to thinning and horizontal spreading.
[22] Any imbalance of this dynamic equilibrium between mass gain, loss and transport due to flow results in either growing or shrinking ice bodies.
Ice sheets are the greatest potential source of global freshwater, holding approximately 77% of the global total. This corresponds to 80 m of world sea-level equivalent, with
Antarctica accounting for 90% of this.
Greenland accounts for most of the remaining 10%, with other ice bodies and glaciers accounting for less than 0.5%. Because of their size in relation to annual rates of snow accumulation and melt, the residence time of water in ice sheets can extend to 100,000 or 1 million years. Consequently, any climatic perturbations produce slow responses, occurring over glacial and interglacial periods. Valley glaciers respond rapidly to climatic fluctuations with typical response times of 10–50 years.
[23] However, the response of individual glaciers may be asynchronous to the same climatic forcing because of differences in glacier length, elevation, slope, and speed of motion. Oerlemans (1994) provided evidence of coherent global
glacier retreat which could be explained by a linear warming trend of 0.66 °C per 100 years.
[23]
While glacier variations are likely to have minimal effects upon
global climate, their recession may have contributed one third to one half of the observed 20th Century rise in sea level (Meier 1984; IPCC 1996). Furthermore, it is extremely likely that such extensive glacier recession as is currently observed in the Western Cordillera of North America,
[24] where runoff from glacierized basins is used for
irrigation and
hydropower, involves significant hydrological and
ecosystem impacts. Effective water-resource planning and impact mitigation in such areas depends upon developing a sophisticated knowledge of the status of glacier ice and the mechanisms that cause it to change. Furthermore, a clear understanding of the mechanisms at work is crucial to interpreting the global-change signals that are contained in the time series of
glacier mass balance records.
Combined
glacier mass balance estimates of the large ice sheets carry an uncertainty of about 20%. Studies based on estimated snowfall and mass output tend to indicate that the ice sheets are near balance or taking some water out of the oceans.
[25] Marinebased studies
[26]suggest sea-level rise from the Antarctic or rapid ice-shelf basal melting. Some authors (Paterson 1993; Alley 1997) have suggested that the difference between the observed rate of sea-level rise (roughly 2 mm/y) and the explained rate of sea-level rise from melting of mountain glaciers, thermal expansion of the ocean, etc. (roughly 1 mm/y or less) is similar to the modeled imbalance in the
Antarctic (roughly 1 mm/y of sea-level rise; Huybrechts 1990), suggesting a contribution of sea-level rise from the Antarctic.
Relationships between global climate and changes in ice extent are complex. The mass balance of land-based glaciers and ice sheets is determined by the accumulation of snow, mostly in winter, and warm-season
ablation due primarily to net radiation and turbulent heat fluxes to melting ice and snow from warm-air advection,
[27][28](Munro 1990). However, most of
Antarctica never experiences surface melting.
[29] Where ice masses terminate in the
ocean, iceberg
calving is the major contributor to mass loss. In this situation, the ice margin may extend out into deep water as a floating
ice shelf, such as that in the
Ross Sea. Despite the possibility that global warming could result in losses to the
Greenland ice sheet being offset by gains to the
Antarctic ice sheet,
[30] there is major concern about the possibility of a
West Antarctic Ice Sheet collapse. The West Antarctic Ice Sheet is grounded on bedrock below sea level, and its collapse has the potential of raising the world sea level 6–7 m over a few hundred years.