2.1. Surface form and extent

While the general form of the surface of the Greenland ice sheet was known reasonably well in 1936, the central region of the Antarctic ice sheet was not explored until almost 20 years later.

In Figure 1a, we show Reference WagerWager's (1933) contouring of the Greenland ice sheet based on sledge journeys up to 1931, with modifications to include results in Reference LindsayLindsay (1935) of his crossing in 1934. Displacement of the 3000 m contour of central Greenland towards the east was attributed to the greater height and fewer gaps along the mountains on the east coast. Figure 1b is based on Reference Mock and WeeksMock and Weeks (1965) and a Danish Geodetic Survey map of the same date. It shows the present map of the ice sheet north of lat. 72 N., while to the south it agrees broadly with the more recent and detailed map of Figure 3a. Flow lines normal to the general contours are also shown on Figure 1b.

Fig. 1. The Greenland ice sheet.

a. Surface form of ice sheet and exploratory journeys (short-dashed lines) from 1936 based on Reference WagerWager (1933) in Reference Wright and PriestleyWright (1937) with additional route and elevations from Reference LindsayLindsay (1935).

b. General surface form used in 1986 based on Reference Mock and WeeksMock and Weeks (1965) and the 1965 Danish Geodetic Survey map with addition of flow lines assumed normal to contours.

Little was known of the ice sheet of central Antarctica in 1936. A few explorers of the heroic age published perceptive deductions but no-one had crossed the continent. One-third of the coastline had not even been seen. Reference GouldGould (1940) summarized what was known, noting that sledge journeys and flights had “all told, penetrated but a small part of this vast reservoir of ice. It remains still to be explored.” Comparison of his flow-line map of Figure 2a with that of Reference DrewryDrewry (1983) shows that intuition and extrapolation are no substitute for exploration. The 1983 map was compiled from 101 000 elevation measurements from tractor traverses, aircraft flights, and surface elevations measured from randomly drifting balloons. The main ice divide of East Antarctica in Figure 2b is seen to be more central than in Figure 2a, and around 1000 km closer to the Indian Ocean than where it was believed to be a few years after the Society was founded.

Fig. 2. The Antarctic ice sheet.

a. Known and postulated coastline and estimated flow lines from Reference GouldGould (1940) interpreted from data available 50 years ago.

b. Current map of surface form and flow lines from Reference DrewryDrewry (1983).

2.2.1. Satellite altimetry

The use of satellite altimetry, first from Seasat as described in Reference Brooks, Brooks, Campbell, Ramseier, Stanley and ZwallyBrooks and others (1978), now provides a means of mapping the ice-sheet surface in great detail at high accuracy. So far, the data available lie between lat. 72 north and south, the orbital limits of Seasat. After 1989, data to lat. 82° should become available when the satellite ERS-1 is launched. Figure 3a, from Reference Zwally, Zwally, Bindschadler, Brenner, Martin and ThomasZwally and others (1983), shows 100 and 50 m surface contours of the Greenland ice sheet south of lat. 72 °N. Similar maps have been produced for parts of the ice sheet in East Antarctica.

Fig. 3. Surface elevation of the Greenland ice sheet from satellite altimetry.

a. Surface elevations from Seasat radar altimetry showing 100 m contours to 2400 m and 50 m contours above that level. Delineation of major drainage basins based on surface topography by R.A. Bindschadler (from Reference ZwallyZwally, 1984).

b. 10 m contours in the vicinity of the central ice divide near Crete station (CR on map). Dotted tracks show data points used for contouring. Based on an unpublished map of Cundestrup.

Figure 3b shows a more detailed map in the vicinity of the ice divide of central Greenland around Crete station (lat. 71°07'N., long. 37°19'W.). Data for Figure 3a and b come from unmanned orbiting satellites at a density two or three orders of magnitude greater than data used for Figure 1b that came from the few traverses made in 1936.

The relative sharpness of the central ice divide and the smoothness of the surface in this region shown by the 10 m contours are shown clearly on Figure 3b. Since similar deviation from a straight line of the 100 m contours on Figure 3a represents a surface irregularity ten times greater than on Figure 3b, we can see that the surface undulations increase in magnitude considerably as one moves away from the ice divide. This is due to longitudinal stress gradients that increase with ice velocity and bedrock roughness away from divides. Reference MclntyreMclntyre (1985) has mapped such changes over much of the Antarctic ice sheet.

An important development is the planned use of satellites to monitor changes of the surface level of ice sheets to within a fraction of 1 m in order to determine where they are increasing or decreasing in volume.

2.2.2. Satellite imagery

Radiometers have been in operation for 25 years and now operate over many spectral bands between 0.2 μn and 50 μm. Since 1972, scanning micro-wave radiometers have revealed unexpectedly stable patterns of emissivity which have allowed useful extrapolation from the still sparse network of surface data on snow properties. Because the mean annual temperature and the accumulation rate of dry polar firn mainly determine the grain-sizes upon which the micro-wave emission depends, these two parameters account for the main features of the patterns observed over Greenland and Antarctica (Reference Chang, Chang, Gloersen, Schmugge, Wilheit and ZwallyChang and others, 1976).

The Landsat series of satellites has contributed more to the knowledge of ice sheets than any other spacecraft before or since. Apart from early geographical discoveries (Reference MacDonaldMacDonald, 1976), Landsat images have been used to identify and to provide data for planimetric mapping of the contemporary position of ice fronts, ice walls, grounding lines, surface features which can be used to define glacier units, ice streams, the direction of ice movement, crevassed areas which indicate regions undergoing rapid deformation, ice divides as defined by ridges, superimposed ice, surface-equilibrium zones, ablation areas, and glacier surges (Reference SwithinbankSwithinbank, 1985). The long-term average rate of movement of ice streams and ice fronts has been determined from time series of Landsat images. Large areas of blue (bare) ice have been discovered which are likely to be fruitful in the search for meteorites (Reference Whillans and JohnsenWilliams and others, 1983).

3.1. Geophysical surveys

Knowledge of the thickness of ice sheets in 1936 is adequately covered by Reference FlintFlint's (1947) statement that the ice thickness was “almost wholly a matter of conjecture”. For example, after noting the surface slope necessary to make the Greenland ice sheet flow outward, Reference CrollCroll (1879) applied this slope to Antarctica to calculate an ice thickness of 7 miles [11000 m] at the South Pole, but gave 3 miles [4800 m] as a reasoned guess. Reference DalyDaly (1934) had suggested from geological evidence that the Wisconsin ice sheet had been 3000-4000 m thick. More typical estimates of mean ice thickness around 50 years ago were as low as 300-400 m for Greenland (Reference KrügerKrüger, 1929), while for Antarctica a maximum mean thickness of 600 m was often conjectured (Reference FlintFlint, 1947; Reference Odell and SimpsonOdell, 1952).

The little evidence available in 1936 that has stood the test of time came from Reference RossJames Clark Ross (1847), who appreciated that the floating front of the Ross Ice Shelf was probably more than 1000 feet [300 m] thick, and others such as Reference WrightWright and Priestley (1922), who suggested a mean thickness of the ice shelf of 600-750 feet [200 m]. Wegener's Greenland expedition of 1930-31 (Reference SorgeSorge, 1933) made ten seismic ice-thickness measurements that showed bedrock fell back to within a few hundred metres of sea-level up to 120 km inland of the west coast mountains beneath ice up to 1850 m thick. Another measurement at Eismitte suggested a thickness of 1900 m (bedrock + 1100 m), although they questioned this figure because of instrumental difficulties. Their measurements and those of Byrd's 1934-37 Antarctic expedition (Reference PoulterPoulter, 1947) were not widely accepted by Earth scientists, while conjectures about the thickness of ice sheets had varied widely.

It was not until better seismic equipment became available after World War II that Expeditions Polaires Franchises in Greenland from 1948 to 1951, and the Norwegian-British-Swedish Expedition (1949-52) in Antarctica produced convincing measurements (e.g. Reference Holtzscherer and RobinHoltzscherer and Robin, 1954) showing thicknesses of ice sheets up to 3 km. The advent of the International Geophysical Year of 1957-58 then started a concerted international study of the Antarctic ice sheet that still continues. Seismic traverses were carried out by teams from Australia, Belgium, France, Japan, U.K., U.S.A., and the U.S.S.R. By 1970, these totalled more than 50 000 km and gave a general picture of the thickness and bedrock relief of the ice sheet. Early maps by Reference Thiel, Wexler, Wexler, Rubin and CaskeyThiel (1962) and in the Soviet Atlas of Antarctica (Reference BakayevBakayev, 1966) showed most major features that are now known. During these traverses, seismic measurements of ice thickness taken at intervals of 30-50 km were usually supplemented by gravity measurements at one-tenth that spacing to give a more detailed ice-thickness profile. These also showed that the Earth's crust was in approximate isostatic equilibrium with the ice loading (Reference Bentley and OddishawBentley, 1964), in contrast with parts of the Northern Hemisphere where isostatic rebound is still taking place.

3.2. Radio echo-sounding

The technique of radio echo-sounding of ice thickness, first demonstrated by Reference Waite and SchmidtWaite and Schmidt's (1962) use of a 440 MHz radio-altimeter to sound Antarctic ice shelves during the IGY, led to specific development of ice-sounding equipment by Evans in the Scott Polar Research Institute, Cambridge, and others. The principles and application of the technique have been described by Reference Robin, Robin, Evans and BaileyRobin and others (1969) and by Reference Bogorodskiy, Bogorodskiy, Bentley and GudmandsenBogorodskiy and others (1985). Antarctic expeditions using the technique include Australia, Britain, Japan, the U.S.S.R., while the most extensive surveys were made by the joint programme of the U.S. National Science Foundation, the Scott Polar Research Institute, and the Technical University of Denmark (see Fig. 4). Their results now cover half of the Antarctic continent with a grid spacing of 100 or 50 km, while around one-third of the continent remains to be mapped at this density. Results are presented in Reference DrewryDrewry (1983), who estimated the mean thickness to be 2160m compared to Reference Thiel, Wexler, Wexler, Rubin and CaskeyThiel's (1962) seismic-based estimate of 1810 m. Sounding of the Greenland ice sheet has been less extensive, but again confirms the general features found by seismic surveys.

Fig. 4. Radio-echo profile from central Antarctica along the flow line AB of Figure 5. Flow starts from an ice divide to the right of the margin at 230 km. On the left is a sub-ice “lake” near Vostok. Velocities of movement shown above the profile are estimated from a steady-state flow model and are consistent with that measured astronomically at Vostok.

Most thicknesses measured by seismic and gravity sounding agree with radio-sounding results and with spot measurements at three deep bore holes drilled to bedrock. Errors in picking seismic reflections on noisy seismic records occurred in several cases, and some internal radio reflections from within ice shelves have been wrongly interpreted as bottom echoes. A few differences of less than 100 m probably indicate that radio and seismic energy can be reflected from different horizons near bedrock.

3.3. Ice volume

Reference LoeweLoewe (1935) estimated the total volume of the Greenland ice sheet at 2.3 × 10⁶km³. Fifty years of subsequent research have raised the figure to 2.6 × 10⁶km³, an increase of 13% (Reference Budd, Budd, Jacka, Jenssen, Radok and YoungBudd and others, 1982). Before the IGY, Reference BauerBauer (1955) estimated the volume of the Antarctic ice sheet to be 18.9 × 10⁶km³. The IGY seismic traverses (Reference Thiel, Wexler, Wexler, Rubin and CaskeyThiel, 1962) served to raise the figure to 24.3 × 10⁶ km³ and subsequent radio echo-sounding has added a further 24% to yield the current figure of 30.1 × 10⁶km³ (Reference DrewryDrewry, 1983) although Reference Radok, Radok, Brown, Smith, Budd and JenssenRadok and others (1986) give 24.4 × 10⁶km³.

4.1. Introduction

This section presents a range of glaciological and related field measurements which provide the factual basis of our perceptions of ice sheets. We deal separately with laboratory studies needed for development of theories and the resultant theories and hypotheses. These govern perceptions at a different level which may be more penetrating and can provide a unified picture of many field and laboratory studies.

4.2. Surface net balance

Although Reference SorgeSorge (1935) had earlier recognized annual snow strata in Greenland, the stratigraphical method of determining rates of snow accumulation did not come into its own until the pioneering studies of Reference SchyttSchytt (1957) in the Antarctic and Reference BensonBenson (1961) in Greenland. These demonstrated that annual strata could be recognized even in the dry snow parts of ice sheets. A modern accumulation map of the Greenland ice sheet (Reference ReehReeh, 1985) reveals rates varying from 150 kg m^-2 a^-1 in the north to 2500 kg m^-2 a^-1 in the extreme south. With this range it is little wonder that no earlier spot measurements could be used to derive a representative value for the whole ice sheet. Dividing the total accumulation (486 Gt a^-1) by the area of the ice sheet (1.7 × 10 km^-2 s²) yields a mean accumulation rate of 286 kg m^-2 a^-1. Estimates for mean accumulation over the Antarctic ice sheet have ranged from a low of 70 kg m^-2 a^-1 (Reference MeinardusMeinardus, 1938) to a high of 200 kg m^-2 a^-1 (Reference KosackKosack, 1956), though most estimates are now close to 150 kg ^-2 a^-1 (e.g. 143 kg m^-2 a^-1 Reference Giovinetto and BentleyGiovinetto and Bentley, 1985). Extreme values in Antarctica range from over 1000 kg m^-2 a^-1 to 25 kg m^-2 a^-1 at high altitudes in central Antarctica.

Two major factors influencing the distribution of accumulation over ice sheets are seen when this is mapped. The first are the orographic effects which cause heavier snowfall where up-slope winds are predominant, as on the western half of Greenland (e.g. Reference SchyttSchytt, 1974). The second is that the saturation water-vapour pressure of the free air exerts a major control on snowfall. At -40 °C this varies and is approximately halved for each 5 deg decrease of temperature. In free air above the surface inversion, the moist adiabatic lapse rate is around 0.6 deg/100 m altitude. We therefore expect accumulation to halve for each 830 m increase of surface elevation, a figure that applies approximately over East Antarctica above say 1500 m. Effects of latitude and continentality on temperature and precipitation tend to be obscured by orographic effects.

The above argument has been applied to the variation of accumulation with time as well as location. During an ice age when global air temperatures fell by around 5 deg, we should therefore expect net accumulation over central Antarctica to be halved (Reference RobinRobin, 1977). This has been confirmed by data from the Vostok ice core discussed in section 6 (Reference Lorius and LoriusLorius and others, 1985; Reference Yiou, Yiou, Raisbeck, Bourles, Lorius and BarkovYiou and others, 1985).

4.3. Basal net balance

Although observations are few, we now know from related studies of temperature gradients and of the structure of basal ice and its debris content that both melting and freezing occur at the base of the ice sheet. This is due to geothermal and frictional heating and freezing by thermal conduction in certain conditions. Reference ZotikovZotikov's (1963) analysis suggests that melting averaging 2 or 3 mm a^-1 takes place under a region approaching half the area of the Antarctic ice sheet while elsewhere bedrock is frozen. This gives a mean value of basal melting of the order of 1% of surface accumulation. For Greenland the proportion is much less.

In contrast with the above, basal melting and freezing beneath ice shelves can exceed the surface net balance. There is considerable transfer of ice mass associated with latent-heat transfer by ocean currents beneath the ice. It is the counterpart of atmospheric transfer of ocean water evaporated into the atmosphere and later deposited as snow on ice sheets. When the temperature of ocean water moving beneath ice shelves is above the freezing point of sea-water, basal ice is melted. The freezing point is pressure-dependent and ranges from about -1.9 °C at atmospheric pressure to about -2.8 °C under an ice shelf 1200 m thick, depending on salinity. Latent heat absorbed in melting ice beneath a thick ice shelf can be liberated with ice re-forming as water moves from high-pressure (deeper) regions to lower pressures (Reference DoakeDoake, 1976). Both temperature and ice-core analyses suggest that up to 0.5 m a^-1 is added by the process beneath some parts of the Amery and Ronne Ice Shelves (Reference MorganMorgan, 1972; Reference Engelhardt and DetermannEngelhardt and Determann, 1987). However, net overall melting must occur, and this has been estimated at 30-50% of the total mass input to the Ross Ice Shelf and up to 70% of that to the Filchner-Ronne Ice Shelves (Reference DoakeDoake, 1985). Although the possibility of extensive basal melting was recognized by some workers up to 1960, for example, in Reference BuynitskiyBuynitskiy (1960), it was largely overlooked for the next two decades. Attention has again been given to the problem during the current decade by both glaciologists, such as Reference Potter, Paren and JacobsPotter and Paren (1985) whose measurements show a mean melting rate of around 2 m a^-1 beneath George VI Ice Shelf, and by shipborne measurements of salinity and temperature changes with depth off the fronts of the Filchner-Ronne Ice Shelves (Reference Foldvik, Foldvik, Kvinge, Tørresen and JacobsFoldvik and others, 1985) and the Ross Ice Shelf (Reference Jacobs, Jacobs, Fairbanks, Horibe and JacobsJacobs and others, 1985).

4.4. Mass balance

Over the past 40 years many calculations of the mass balance of contemporary ice sheets have been published. They give a broad indication of magnitudes of annual accretion and loss of mass of the two major ice sheets. The variability of both terms over the two vast ice sheets, together with errors and unknown factors such as melting beneath ice shelves, are such that estimates of the balance between input and loss are of little value. Estimates for Greenland lie within the range 515 ± 115 km³ a^-1 for accumulation, 325 ± 105 km³ a^-1 for melting, and 240 ± 80 km³ a^-1 for iceberg discharge. Over the much larger area of Antarctica, there is less variation between most recent estimates of accretion, mainly because everyone extrapolates from the same data input to cover blank spaces on the map. A figure of around 1800 km³ a^-1 to 2000 km³ a^-1 is most common for total accumulation, while mass losses by discharge to the sea run from around half to double this figure.

While the figures above suggest that we do not know whether these ice sheets are increasing or decreasing in mass, some progress can be reported. Some mass-balance figures for individual drainage basins or regions have much lower proportional errors. Reference Hamley, Hamley, Smith and YoungHamley and others (1985), using satellite-derived ice velocities over part of the IAGP study area of East Antarctica between long. 90 °E. and 135 °E. and north of lat. 80°S., found this part of the ice sheet unlikely to be significantly out of balance (±10%). Reference Budd and SmithBudd and Smith's (1985) recent assessment incorporating much improved data from the previous decade gave losses less than an input of around 2000 km³ a^-1 by 0 to 20%. Reference Shabtaie and BentleyShabtaie and Bentley (1987), however, have shown that basins feeding Ice Streams B and C in West Antarctica have large negative and positive balances, respectively.

Analysis of several deep bore-hole temperature profiles in Antarctica suggests a slightly positive mass balance (Reference RobinRobin, 1970; Reference Ritz, Ritz, Lliboutry and RadoRitz and others, 1982). They indicated that over millennia, mean thickness increases at Byrd Station and Dome C have not exceeded the annual accumulation by more than 20%. Interpretation of 8180 data as a proxy indication of surface temperature leads to a similar conclusion.

4.5. Ice movement: surface

During the past 50 years much research has attempted to answer the question “How fast do polar ice sheets flow?“ Scattered measurements show that the down-slope component of movement increases from close to zero at most ice divides to as much as 7 km a“1 on parts of the fastest outlet glacier (Jakobshavns Isbra, Greenland). Until the development of satellite Doppler-positioning techniques, most measurements were confined to the peripheral parts of the ice sheets where flow could be easily determined in relation to fixed points on rock (Reference SwithinbankSwithinbank, 1963; Reference Bauer, Bauer, Baussart, Carbonnell, Kasser, Perroud and RenaudBauer and others, 1968). Despite enormous difficulties, classical triangulation and trilateration techniques were subsequently used to extend velocity measurements inland (Reference Bauer, Bauer, Baussart, Carbonnell, Kasser, Perroud and RenaudBauer and others, 1968) and away from fixed points (Reference Dorrer, Dorrer, Hofmann and SeufertDorrer and others, 1969). Satellite methods have revolutionized the measurement of ice-surface velocity because they can be used to determine coordinates in three dimensions at any point on an ice sheet. Reference Drew and WhillansDrew and Whillans (1984) claimed position errors of less than 0.2 m close to the ice divide in southern Greenland. A comprehensive set of ice-velocity and thickness data was used to calculate mass balance and ice flow-law parameters over parts of East Antarctica (Reference Hamley, Hamley, Smith and YoungHamley and others, 1985) and at a stake network extending over almost the whole area of the Ross Ice Shelf (Reference Thomas, Thomas, MacAyeal, Eilers, Gaylord, Bentley and HayesThomas and others, 1984).

However, relatively few direct measurements of ice movement have been made over most of the ice sheets. Other evidence from temperature profiles and studies of ice cores confirms to a first approximation that outflow of the ice sheet from central regions is roughly in balance with the surface accumulation over many, but not all, accumulation basins of the ice sheet of Antarctica. More field data from Greenland, as well as Antarctica, along with theoretical modelling and computer analyses are necessary before we will know whether individual basins of the ice sheets are in balance with the ice input.

4.6. Ice movement: internal

There have been few measurements of internal deformation of bore holes in ice sheets to provide comparable information to that from many valley glaciers, mainly in temperate ice. Reference Garfield and UedaGarfield and Ueda (1976) measured the change of tilt of the Byrd Station bore hole from 1968 to 1975. Below around 1100m the changes were in the same azimuth as the surface movement determined by Reference Whillans, Robin and PressWhillans (1983). At smaller depths where tilting was less, it differed by over 90 in azimuth from deeper layers.

Some indication of internal deformation is also given by deformation of internal sedimentary layering seen on radio-echo records (Fig. 4), especially on deep ice of central Antarctica. Reference Robin, Robin, Drewry and MeldrumRobin and others (1977) found that to a first approximation (±10%), vertical strain-rates of the top 80% of the ice column were approximately uniform (±10%), as ice moved over bedrock relief variations of over 1 km in height with ice thickness up to 3.5 km along a 230 km flow-line profile. Slope variations of the lowest layer along the profile were often less than one-fifth of those of the bedrock surface. This indicates that large variations of basal shear must occur at lower levels, in contrast to the relatively uniform vertical strain-rates in cold ice at upper levels. Other records of layer deformation around steep subglacial peaks show a strong deformation in three dimensions, with much of the deformation being preserved in ice further down the flow line (Reference Robin and MillarRobin and Millar, 1982).

4.7. Temperature distribution

Although the extremely low temperatures of surface layers of the ice sheet were so well known to the early explorers, and had been measured to 17 m depth at Eismitte by Sorge and to 41 m by Wade at Little America in 1940, temperatures in the deep interior of the ice sheet received little consideration. Probably, if thought about 50 years ago, it was assumed that everywhere below a certain depth the ice would be at pressure melting-point. The changed perception was stimulated by bore-hole temperature measurements of the French across central Greenland in 1948-51 and by the NBSAE to 100 m depth at Maudheim. The different temperature gradients in different locations were explained to a first order in terms of a steady-state model that took account of downward advection of cold ice. This suggested basal temperatures below freezing point beneath central Greenland (Robin, 1955). At the same IUGG meeting in Rome where this was first presented, Haefeli, on the basis of basal ice stresses and Holtzscherer's seismic refraction shooting results, concluded that the basal ice temperature of central Greenland was below freezing point.

Appreciation that mean temperatures of polar ice sheets could depend more on the surface than basal (melting?) temperature stimulated development of radio echo-sounding techniques. Successful radio echo-soundings in north-west Greenland in 1964 showed the validity of the concept. More direct evidence came when deep bore-hole temperatures to bedrock were obtained at Camp Century in 1966 and at Byrd Station in 1968, the former with a temperature of -13.0 °C 17 m above bedrock, and the latter, as expected, at the pressure melting-point (-1.6 °C). Since this start, more deep bore holes have given further and more accurate data while theory and calculations have been improved to take account of basal melting or freezing, more realistic internal deformation models, and variations with time of the climate, size, and flow of ice sheets. Figure 5 shows 10 m and deep ice temperatures now measured on the Antarctic ice sheet. The varied profiles can all be explained by available theory – at least to a first order. The strongest gradients are found at the base of ice shelves where much melting takes place – the smallest basal gradients are also on an ice shelf (Amery) where basal accretion of ice (see section 4.2) is estimated at around 0.5 m a^-1. Development of computer techniques has made possible close matching of temperature profiles to realistic input figures for accumulation, boundary temperatures, and ice flow (Reference Budd, Budd, Jenssen and RadokBudd and others, 1971). Improvements on first-order calculations have resulted from using a temperature input derived from stable isotopic ratios (δ^l8O) together with better strain-rate/ice-flow modelling (Reference Budd, Young and RobinBudd and Young, 1983; Reference Jenssen, Campbell and RobinJenssen and Campbell, 1983). The improved agreement between computed and observed temperature profiles shows the approximate validity of the use of isotopic values as indicators of past surface temperatures back into the last ice age.

Fig. 5. Antarctic ice sheet, showing elevation contours, isotherms of 10 m depth temperatures (mean annual), and measured temperature-depth profiles (from Reference RobinRobin, 1983). Line AB shows location of radio-echo profiling in Figure 4. Line DE shows the location of the profile in Figure 6.

4.8. Bore-hole sampling of deep ice

Development of ice-coring techniques since 1950 has provided ice-core samples down to bedrock at Camp Century and Dye 3 in Greenland, at Byrd Station, Antarctica, and to similar depths at Dome C and Vostok in East Antarctica. Although the latter two did not reach bedrock, the Vostok core has produced the oldest ice with almost continuous sampling from the surface to 2083 m depth where the ice is around 160 000 years old. We discuss geochemical studies of these ice cores in section 6.

The importance of core samples to ice dynamics comes from provision of material on which deformation studies for determining stress/strain-rate relationships can be carried out. The dependence of this relationship on temperature, crystal structure (crystal size and fabric orientation) can all be determined in the laboratory on field samples as distinct from laboratory-grown ice. This has been particularly important in relation to development of strong crystal orientation that increases the deformation by shear along easy glide planes by a factor of up to five times, while fine-grained crystal fabric resulting from deposition during ice ages also increases deformation rates considerably. Changes of crystal size and an increasingly random orientation in the lowest few hundred metres of the Byrd Station core suggest a lower rate of deformation occurs in the lowest layers – an effect not expected from simple theory.

Another potentially useful parameter obtained from ice cores is measurement of their total gas content. This provides a pressure-altimetric record of the altitude at which air bubbles were trapped in the ice, and hence a record of former surface elevations at which sections of the ice core were deposited (Reference Raynaud and LebelRaynaud and Lebel, 1979; Reference Jenssen and RobinJenssen, 1983). Further verification is needed before we know in which locations such deductions are acceptable.

4.9. Glacial geology

Fifty years ago, concepts on the dynamics of ice sheets were mainly based on observations of glacial geologists. In his book The Quaternary ice age, Reference Wright and PriestleyWright (1937) said, concerning the essential distinction between mountain glaciers and ice sheets, “In the physics of their nourishment and depletion and above all in their physiographical and geological effects, these two types of accumulation exhibit fundamental differences. It might almost be said that they have little in common except the possession of a pseudo-plastic motion under the action of gravity, which is the property of all ice masses large and small”. In 1936, studies of glacial geology were almost entirely confined to evidence of terrestrial deposits and erosion by former ice sheets. Much information has been added during the past 50 years by marine geologists analysing cores obtained from the ocean floor. Instead of three or four Pleistocene glaciations in the Northern Hemisphere, marine geologists have shown that a whole series of glaciations in the Northern Hemisphere started around 2.4 Ma ago. They increased in magnitude around 0.7 Ma. They show dominant periodicities around 100, 40, and 23 ka, which are similar to those of radiation changes at high latitudes due to orbital changes of the Earth in regard to the Sun (Reference Hays, Hays, Imbrie and ShackletonHays and others, 1966).

Another input from some glacial geologists and some physical glaciologists is the direct study of carriage and deformation of basal till within and beneath glaciers. Until recently, such studies beneath ice sheets were limited to examining basal layers in cores from the few drill holes that have reached bedrock. Recently, seismic studies in Antarctica have shown that deformation of very soft till beneath Ice Stream B in Byrd Land (Reference Blankenship, Blankenship, Bentley, Rooney and AlleyBlankenship and others, 1986) can explain the high surface velocities. Evidence of block transport of large amounts of soft till beneath former ice sheets of Europe over considerable distances may also be due to rapid deformation within the till.

During the past 40 years, measurements of processes and theoretical advances in ice dynamics have dominated the attention of physical glaciologists to such an extent that, with a few notable exceptions (see Reference BoultonBoulton, 1987), the potential contributions of glacial geology to our understanding of ice dynamics have been overlooked.

5.1. Introduction

In order to understand the links between different observations on ice sheets we need to develop theories of ice dynamics. These should cover various aspects of their flow, form, and interactions with the atmosphere, oceans, and solid earth. We should then be able to use the theories to improve interpretation of evidence of former glaciations, to predict future changes of ice cover and its role in the future global climate. We are unlikely to do this effectively until we have a comprehensive understanding of the dynamics of present-day ice sheets, although a limited understanding can help on some problems. Reference CrollCroll's (1879) estimate of ice thickness at the South Pole is one early example.

A simple assumption is that since the basic physics of ice does not change with time, former ice sheets will have had similar characteristics to present-day ice sheets, especially the relationship of volume to area. On this basis, Reference Donn, Donn, Farrand and EwingDonn and others (1962) estimated sea-level lowering during the last glacial maximum from the known area of former ice sheets and hence their volume. Their figure for sea-level lowering of 137-159 m agrees roughly with subsequent evidence from ¹⁴C dating of submerged beaches and coral reefs. Such a general relationship is not, however, applicable everywhere. When basal sliding occurs or when ice is carried along on deforming basal sediments, ice-surface slopes and hence ice-sheet volumes can be much smaller. Until we have better theories of basal sliding and of deformation of sub-ice sediments and of their consequent interaction on the internal deformation of ice sheets, our knowledge of the dynamics of ice sheets will not provide a satisfactory basis for forecasting. The same is true to a lesser extent in regard to the internal deformation of ice masses.

5.2. Extrusion flow and later theories

Fifty years ago the concept of extrusion flow was receiving attention. In the first issue of the Journal of Glaciology (Vol. 1, No. 1, 1947, p. 12-21), a paper “Extrusion flow on glaciers” recorded a discussion of 26 April 1946 led by Seligman. High pressures at depth in glaciers were believed to cause ice to deform more easily so that it was extruded under the weight of overlying ice. Reference DemorestDemorest (1943) postulated that the enormous ice streams of the Greenland fjords must be fed by extrusion from the centre of the ice sheet. Reference Streiff-BeckerStreiff-Becker (1938) considered the measured accumulation on a Swiss glacier was being carried away more quickly than was indicated by measured surface flow, which pointed to extrusion flow.

To test the extrusion-flow hypothesis, the technique of measuring changes with time of the tilt of a vertical bore hole was developed (Reference PerutzPerutz, 1950) in order to determine the vertical distribution of the down-slope velocity of glaciers. This led to rejection of the extrusion-flow hypothesis and was one of several major changes affecting our perception of ice sheets during the following decade. Another factor helping these changes was the increased use of steady-state models since 1950 which made it possible to produce analytical solutions to problems of ice dynamics and thermodynamics. In these solutions, parameters such as accumulation rate, thickness, velocity, and temperature do not change with time at any point in a glacier or ice sheet. This concept, along with much improved information on the physical properties of ice, stimulated various changes. Careful laboratory studies of the deformation properties of polycrystalline ice, first by Glen (1955), and then by others, showed that strain-rates varied as the third or fourth power of the applied stress as well as being strongly dependent on temperature. Field studies confirmed these findings and led to the introduction of new theories treating ice as a plastic material or with a realistic flow law instead of the linear relationship of Newtonian viscosity. Nye (1951) pointed out that the relevant stresses were, as in metallurgy, the deviatoric stresses and that hydrostatic stresses had little or no effect. Rigsby (1958) showed this to be the case by laboratory experiments.

Nye (1951, 1952) showed that the thickness (h) of an ice sheet at any point was inversely proportional to surface slope (a) and that the basal shear stress (τ_b) was given by

(1)

This result was derived from both plastic and Glen's flow laws and has dominated glaciological theory since its introduction. Prior to use of surface slopes in Equation (1), the role of bottom slopes and the down-slope component of weight on bedrock received more attention. Both approaches are now used, although emphasis on the role of bedrock is largely confined to theories related to mountain glaciers. Field results from ice sheets showed that Equation (1) only applies to mean slopes over distances an order of magnitude greater than the ice thickness. At shorter distances, the surface slope of ice sheets is strongly influenced by gradients of longitudinal stress, as shown by theoretical and field studies around 1967-71. Values of τ_b, which usually lie between 0.5 and 1.5 bar (50-150 kPa) on most glaciers and ice sheets, fall to much lower values on rapidly flowing ice streams and outlet glaciers of the Antarctic ice sheet and to zero beneath floating ice shelves. Deformation is then related to principal deviatoric stresses σ_x’, σ_y’ σ_z’ (x-axis in the flow direction – horizontal or tilted parallel to the mean surface or basal slope). A theory of1 ice-shelf flow linked to Glen's law was presented by Reference WeertmanWeertman (1957[a]), and modified by Reference BuddBudd (1966), Reference ThomasThomas (1973[a], Reference Thomas[b]), and Reference SandersonSanderson (1979) to take account of lateral and other restraining forces. A forerunner to these modifications was Reference CraryCrary's (1966) “Mechanism for fjord formation indicated by studies of an ice-covered inlet”.

5.3. Sliding and internal deformation

The question of how much the motion of large ice sheets is due to internal deformation and how much to sliding has not been fully solved. It is clear that fast motion of ice streams and trunk glaciers is dominated by sliding as surface slopes are too small to generate stresses needed to produce observed surface velocities by internal deformation. An empirical plot of many ice-surface velocities (V _i) divided by ice thickness (z) by Reference Budd and SmithBudd and Smith (1981) was related to basal shear stress τ_b by

(2)

where n and K come from Glen's relation and is the mean shear rate through the ice column if there is no basal sliding. A plot of data from a variety of sources on polar ice gave n = 3.5 and K = 0.025 bar^-n m^-1. Reference Hamley, Hamley, Smith and YoungHamley and others (1985), using data from a sector of East Antarctica between Dome C and the coast, gave n = 3.21 and K = 0.023 bar^-n m^-1. The values of n are close to those of Glen and many values derived from internal deformation of glaciers, while that for K is that to be expected of polycrystalline ice some degrees below freezing point. If the motion had been dominated by sliding, we would have expected a relationship such as V _i α τ_b ² based on the sliding theory of Reference WeertmanWeertman (1957[b]) and others or V _iZ* α τ_b ³ (Reference Budd and SmithBudd and Smith, 1981) based on laboratory experiments where Z* is the equivalent normal stress on the bed (weight of overlying ice minus basal water not change with time at any point in a glacier or ice sheet. This concept, along with much improved information on the physical properties of ice, stimulated various changes. Careful laboratory studies of the deformation properties of polycrystalline ice, first by Reference GlenGlen (1955), and then by others, showed that strain-rates varied as the third or fourth power of the applied stress as well as being strongly dependent on temperature. Field studies confirmed these findings and led to the introduction of new theories treating ice as a plastic material or with a realistic flow law instead of the linear relationship of Newtonian viscosity. Reference NyeNye (1951) pointed out that the relevant stresses were, as in metallurgy, the deviatoric stresses and that hydrostatic stresses had little or no effect. Reference RigsbyRigsby (1958) showed this to be the case by laboratory experiments.

Reference NyeNye (1951, Reference Nye1952) showed that the thickness (h) of an ice sheet at any point was inversely proportional to surface slope (a) and that the basal shear stress (τ_b) was given by pressure). Although it is clear from observation of sub-ice water masses that τ_b varies widely at the bed of polar ice sheets (Reference Whillans and JohnsenWhillans and Johnsen, 1983), flow of the inland section of major ice sheets does appear to be dominated by internal shear deformation within the lower layers of ice, as described in Reference NyeNye (1959), while the principal stresses are dominant in upper layers. The resultant deformation is not that different from sliding at an interface, since we have very strong shear deformation in the lowest 10% or so of the ice sheet, but little shear in upper layers where longitudinal deformation is dominated by principal stresses.

The transition from motion by internal shear to motion by sliding frequently takes place where ice enters trunk glaciers and moves from a roughly horizontal bed over a steep bedrock scarp which is effectively the headwall of an ice-filled fjord (Reference MclntyreMclntyre, 1985). The observed presence of extensive water at the base of the ice on radio-echo records near this point, as well as the sharp decrease of surface slope down-stream, both indicate the onset of sliding. Association of this onset of sliding with a sudden increase of bedrock slope is not covered by accepted theories of sliding which require modification. Similarly, too much weight should not be given to numerical values of K obtained by empirical fitting of observations to Equation (2), since other effects than temperature operate, such as easy gliding with a strongly oriented crystal fabric or changes of ice rheology with crystal size and dust content.

5.4. Surging

No glaciers or ice sheets are in a completely steady state, but for many the inter-annual variations cause rather limited changes of flow. Many surging valley glaciers, in contrast, are quiescent over some decades before their flow increases by one or two orders of magnitude for a year or more. The repetitive cyclic surging history of such glaciers suggests that an internal mechanism rather than external forcing is usually the dominant cause, although this is not always the case.

Reference WilsonWilson (1964) suggested that massive surging of the Antarctic ice sheet could take place and be responsible for global ice ages during the Pleistocene. This has stimulated much work, both theoretical and in the field, but no fully convincing field evidence has been provided of such massive surging. Theories and computing models that produce surges have been produced, as well as studies showing that certain types of instability are unlikely. Such theories do not prove or disprove existence of massive surges of continental ice sheets or the correctness of the theories. Field evidence from temperature and isotopic profiles in polar ice sheets provide no support for the hypothesis. Dynamic observations thought to provide support for surging of large basins of the Antarctic ice sheet have not withstood further examination. Only one convincing case (Ice Stream C of Byrd Land) of a surge involving a discharge of the order of 10⁴ km³ some 300 years ago has been provided to date. While other cases will no doubt be found in the future, the Ice Stream C surge involved a volume about five times the annual discharge of ice from the continent or around 0.04% of the total mass of the ice sheet. This is of little climatological significance.

5.4. Publications

It is impracticable in a review of this length to do justice to all the theoretical laboratory and computing studies that have advanced our knowledge of glaciology rapidly during the past four decades. Perceptions of ice physicists have resulted from laboratory work as well as theoretical models, those of mathematicians from more complex and mathematically rigorous approaches, and by improving knowledge of boundary conditions. Much remains to be done.

Widespread changes of perception are perhaps shown most clearly when knowledge moves from the realm of research papers to its incorporation in textbooks for students and research workers. An exhaustive list would be invidious, but textbooks that include substantial discussions on the dynamics of ice sheets include those by Reference ShumskiyShumskiy (1964), Reference LliboutryLliboutry (1964-65), Reference PatersonPaterson (1969, 1981), Reference ColbeckColbeck (1980), and Reference HutterHutter (1983). Books that record advances in knowledge of the basic physics and physical chemistry of ice include Reference DorseyDorsey (1940), Reference PounderPounder (1965), Reference FletcherFletcher (1970), and Reference HobbsHobbs (1974).

5.5. Modelling studies

The rapidity with which one can set up finite-element or other other models to provide numerical answers from glaciological theories has contributed to our understanding of ice sheets in recent years. The main value of a computing study is usually in the evidence it gives on the effect of changing certain parameters or of the relationship between several parameters. Furthermore, the results can be no better than the information fed into the models, and this can be unsatisfactory as mentioned in section 5.3 in relation to sliding and surging glaciers.

An outstanding early computing study was “The derived physical characteristics of the Antarctic ice sheet” by Budd and others (1970). Figure 6 from this study illustrates some points in the preceding paragraph. They used a simplified moving vertical column model, the steady-state assumption applied to the present surface and bedrock profiles, and all available information on the present surface-accumulation rates and temperature. The results show the resultant particle trajectories, temperature-depth profiles, and isochrons of former surface layers in later millennia.

Fig. 6. Calculated particle paths (arrows), isochrones (dashed lines, ages in 10³ a), and temperature–depth profiles (full lines, temperatures in °C), assuming steady-state conditions along profile from Vostok to Wilkes Station (from Reference Budd, Budd, Jenssen and RadokBudd and others, 1971).

The temperature-depth curves in Figure 6 provide a good qualitative and a rough semi-quantitative three-dimensional fit to the temperature observations in Figure 5. The shape of the isochrons is similar to the radio-echo layering of Figure 4. This provides an impressive justification of the theory of ice dynamics used as a basis for modelling. However, calculated basal temperatures from 0 to 900 km are well below freezing point, whereas radio echo-soundings in the region of Vostok indicate the presence of extensive basal melting and sub-ice water. The discrepancy appears to be due mainly to use of too high values of accumulation rate in modelling. More recent figures from field measurements would have predicted basal melting. Some changes of ice thickness and uncertainty over values of geothermal and frictional heat supply also add uncertainty to numerical values from modelling. Unfortunately, the above modelling results led to the proposal that, because the base of the ice sheet of central Antarctica was frozen, it would be a suitable place for dumping radioactive waste with a long half-life – a proposal that was dropped when later evidence became available.

Reference WhillansWhillans (1976) also showed the value of modelling studies, even though the final answer was not fully satisfactory on a quantitative basis. He used similar input parameters to Reference Budd, Budd, Jenssen and RadokBudd and others (1971) for Figure 6, together with his measured surface velocity and strain-rate data on the flow line leading to the Byrd Station bore hole. Whillans’ calculated shapes of the 30 ka and other isochrons showed good agreement with the observed form of radioecho layering along the same 300 km profile. It was concluded that the thickness and flow of the ice sheet had not changed to any extent over the past 30 ka. While this is probably correct regarding thickness and form of the surface and isochrons, later studies suggest that the dating and flow rates may well be out by up to 50%.

Similar problems arise with modelling of former ice sheets. Reasonable limits to the rates of growth and decay of Pleistocene ice sheets can be computed on the basis of probable input parameters, but results are not precise (Reference WeertmanWeertman, 1964). Basal temperatures and related erosion patterns can be computed on a broad regional basis. The effect of isostatic rebound in accelerating retreat of large Northern Hemisphere ice sheets can also be shown semi-quantitatively (Reference Budd and SmithBudd and Smith, 1981). It is clear that as our basic knowledge of the flow and other physical properties of ice sheets improves, our ability to produce models of past and future ice sheets and their response to global forcing by, say, increased atmospheric CO², will also be improved. However, this will result more from a better understanding of all the physical processes associated with the nourishment, flow, and wastage of present-day ice sheets than from further improvements in computing techniques. We need continued and increasing field studies including techniques such as core drilling and satellite studies of ice velocity and elevation changes. Studies in the field, laboratory, and computing rooms, will all require use of increasingly sophisticated techniques. The geochemical studies of the next section show the rewards of such advances.

6.1. Introduction

Fifty years ago we lacked adequate geographical knowledge of the characteristics of the Antarctic ice sheet. Apart from filling this gap, ice-sheet studies are now providing unique data of interest to a much wider group than polar scientists. Research into many global problems, especially in geophysics, shows that studies on a regional basis are often unsatisfactory. Answers do not become clear until a global pattern has been obtained. Furthermore, studies of polar ice sheets now provide certain data of global importance of a quality and/or quantity that are not available elsewhere. We shall discuss the global importance of studies of ice sheets briefly in three major fields:

1. (1) Global climate.

2. (2) Geochemistry.

3. (3) Other geophysical sciences.

6.2. Ice sheets and climatology

Data from ice sheets are important to climatology in two ways. Ice sheets are a stabilizing component of the atmosphere-ocean-cryosphere system with a long response time that resists rapid changes. When dynamic modelling of climatic systems is fully developed, it must include the atmosphere, ocean, and ice sheets, and the interaction between these components. At present, dynamic models of these three major components are not yet sufficiently developed in their own medium, and this does not justify confidence in models linking all three in a joint model. On the longer time-scales of importance for global climatology, present models of ice dynamics may be considered as better developed than those of oceanography and possibly also those of atmospheric dynamics.

The second aspect important to climatology is provided by the very detailed record of past climates preserved in ice sheets on a time-scale ranging from annual variability to 10⁵ and even 10⁶ years. Internal layering in the Greenland ice sheet measured in isotopic profiling of ice cores has recorded annual variations of accumulation over the past 800 years (Reference Hammer, Hammer, Clausen, Dansgaard, Gundestrup, Johnsen and ReehHammer and others, 1978) and in future similar detail is likely over at least ten times that period. Similarly, proxy temperature records from δ¹⁸O and δD profiles already cover the last 1.5 × 10⁵ years, and this is likely to be extended to three to six times that figure during the next few years. Limitations to the accuracy of climatic parameters deduced from such records have been discussed at length by Reference RobinRobin (1983). In spite of these limitations, which are probably better understood than those of other proxy records, there appears to be no other marine or terrestrial evidence with comparable resolution on the time-scale of 10³ to over 10⁵ years.

The value of stratigraphic profiling of isotopic, chemical, ice-fabric, and other parameters was shown by Lang way's (1970) discussion of results from a 411m core at Site 2 in north-west Greenland. Isotopic profiles down to bedrock were first measured in Copenhagen by Reference Dansgaard, Dansgaard, Johnsen and MollerDansgaard and others (1969) on a 1388 m ice core from Camp Century and by the same group (Reference Johnsen, Johnsen, Dansgaard, Clausen and LangwayJohnsen and others, 1972) on a 2164 m ice core from Byrd Station. Drilling of these cores has been described by Reference Hansen and LangwayHansen and Langway (1966) and Reference Ueda and GarfieldUeda and Garfield (1970), respectively.

In Figure 7, from Reference Jouzel and JouzelJouzel and others (1987), we show results obtained by scientists from France and the U.S.S.R. from studies of the 2083 m ice core from Vostok station, Antarctica. In this case, the 6D (deuterium) isotope was measured instead of δ¹⁸O profile (δD ≈ 8δ¹⁸O). Measurements were made of the mean isotopic value along 1 m increments of the ice core to give high resolution and a clear indication of noise level along the core. Results of 8D in Figure 7 are expressed as temperature departures from present-day surface temperatures. Dating of the ice core was done entirely by glaciological modelling along similar lines to dating of isochrons in Figure 6. Comparable profiles from studies of marine cores also shown in Figure 7 were dated by quite independent methods of isotopic and magnetic age determination. The close correspondence with ages determined by glaciological dating gives confidence in the latest model of ice dynamics employed, which also included dependence of accumulation rate on atmospheric temperature.

Fig. 7. a. Variation with time of the Vostok isotope temperature record in °C from δD values. The present mean surface temperature of -55.5 °C is shown as 0 °C on the scale. Temperatures are mean values over 100 years (thin lines) along with a smoothed curve (thick line).

b. Variation with time of summer sea-surface temperatures from core RC11-120 in the sub-polar Indian Ocean (from Reference Martinson, Martinson, Pisias, Hays, Imbrie, Moore and ShackletonMartinson and others, 1987).

c. Variation with time of continental ice volume based on benthonic δ¹⁸O records (from Reference Martinson, Martinson, Pisias, Hays, Imbrie, Moore and ShackletonMartinson and others. 1987). (Figure 7 is reproduced from Reference Jouzel and JouzelJouzel and others (1987) by permission of Nature.)

6.3. Atmospheric geochemistry

In Figure 8 we show measurements of the CO² content of air trapped in the ice core over the same period, using techniques developed by Reference Oeschger, Oeschger, Stauffer, Neftel, Schwander and ZumbrunnOeschger and others (1982). No comparable data have been obtained from other media over such a time-scale. In view of concern over the increasing atmospheric CO₂ levels due to Man's use of fossil fuels and the global warming due to the greenhouse effect of CO₂ and other gases, the data of Figure 8 are of great practical value. They should help to show whether CO₂ fluctuations are driven by climatic changes, or the reverse. The record shows that present atmospheric CO₂ levels of around 345 ppm by volume exceed any known levels during the past 150 ka.

Fig. 8. Measured parameters on the Vostok ice core plotted against depth on the bottom scale and against time on the upper (non-linear) scale.

a. Deuterium content (in ‰ w.r.t. SMOW). These data are interpreted as temperature in Figure 7a (from Reference Jouzel and JouzelJouzel and others, 1987).

b. Carbon dioxide concentrations (ppm volume). Dots show the best estimates of CO₂ and the envelope indicates the uncertainty (from Reference Barnola, Barnola, Raynaud, Korotkevich and LoriusBarnola and others, 1987).

c. Aluminium concentration (ng g^-1) (from Reference Angelis, Angelis, Barkov and PetrovDe Angelis and others, 1987).

d. Marine sodium concentration (ng g^-1) (from Reference Angelis, Angelis, Barkov and PetrovDe Angelis and others, 1987).

Studies of other gases, solids, and trace elements trapped in ice cores also provide a wonderfully detailed record of the Earth's atmosphere against a well-calibrated time-scale. For a study of individual events and interactions between different parameters, relative dating errors along sections of an ice core can be very small and of great value. This applies particularly to solids (volcanic ash, terrestrial dust) and conductivity (SO₄) changes which record particular events and can be related to climatic changes recorded in 8180 profiles (Reference HammerHammer, 1980). Changes of concentration of major components of the atmosphere (N₂, O₂, Ar, etc.) (Reference Raynaud and DelmasRaynaud and Delmas, 1977) over 10⁵ years are known to be relatively small, and this provides a useful constraint on atmospheric modelling. The concentrations of certain trace elements such as ¹⁰Be appear to be linked with action of cosmic rays on the upper atmosphere. They show that mean cosmic ray activity over long periods of time have not varied greatly over 10⁵ years, although some periods of enhanced activity seem likely (Reference Yiou, Yiou, Raisbeck, Bourles, Lorius and BarkovYiou and others, (1985).

Studies of dust in polar ice cores have shown how the distribution of microparticles is related to location and weather systems (Reference Thompson and ThompsonThompson and Mosley-Thompson, 1982). Figure 8 shows how amounts of aluminium and sodium varied with time in the Vostok ice core of Figure 7. The aluminium curve is an indicator of dust from terrestrial sources, while the sodium records variations of marine salts (Reference Angelis, Angelis, Barkov and PetrovDe Angelis and others, 1987). Peaks of Al result from increased aridity and exposure of continental shelves of mid southern latitudes, as well as changes of wind strengths which are shown by both curves, as are the influence of changes of accumulation rate.

An extremely important aspect of geochemical studies of polar ice cores is their ability to provide a record of the global effect of man-made changes on the global atmosphere. CO₂ has already been mentioned, while other greenhouse gases such as nitrous oxide (NO₂), methane (CH₄), and chlorofluorocarbons have also been measured in polar ice cores. One great advantage of polar ice cores is that one can measure the variability of these components from natural causes before Man had a significant effect. It is essential to know this background variability before assessing the significance of shorter-period historical records and the global temperature effects of greenhouse gases. Man's increasing injection of lead into the atmosphere from automobile exhausts since 1950 is well recorded in ice cores from Greenland (Reference Murozumi, Murozumi, Chow and PatersonMurozumi and others, 1969). There are no comparable increases of lead in the Antarctic ice sheet, where observed short-period fluctuations are explained by volcanic activity.

The relationship between changes of atmospheric composition of trace elements and gases to those trapped in ice sheets studied by Reference Wolff and PeelWolff and Peel (1985) removes one further uncertainty of interpretation of ice-core data as a long-term historic record of atmospheric changes. Ice coring is logistically difficult and expensive, and the analysis of minute quantities of trace elements in the laboratory demands sophisticated techniques with a very high quality of processing. The results are of such wide importance that further expansion of these studies seems inevitable as Man's concern over modification of the Earth's atmosphere increases.

6.4. Ice sheets and global geophysics

The discovery of a number of meteoritic fragments on a limited area of bare ice near the Yamato Mountains (Reference Yoshida, Yoshida, Ando, Omoto, Naruse and AgetaYoshida and others, 1971) has led to specific searches of other areas where ice flow and ablation could produce surface concentrations of this material. As a result, more meteoritic fragments have been found on the Antarctic ice sheet during the last two decades than the total collected from elsewhere on Earth. Furthermore, since these have remained encased in cold ice since falling on Earth, their chemical purity has been little changed over many millennia compared with similar changes of old meteoritic material from terrestrial or marine sources. Meteorites from the Antarctic ice sheet, now under curatorship in the Smithsonian Museum, Washington D.C., have been distributed to experts in many countries for detailed analysis. This is another encouraging example of serendipity in the study of ice sheets.

Similar carriage and concentration by ice of diatoms has probably confused rather than helped glacial geologists in another field, the interpretation of old diatoms found in the Sirius Formation – altitude -2000 m in the Transantarctic Mountains. It is difficult to explain their location from their terrestrial (lacustrine) or marine origin and by transport by ice without a drastic modification of concepts on the history of Antarctic tectonics and glaciation. This example provides a warning that some basic geophysical and glaciological concepts need further verification.

Carriage of vast loads of basal moraine by polar ice sheets and its eventual deposition on the ocean floor provides valuable information to marine geologists on the global climatic and geological records – another rapidly expanding field of research. However, glaciological knowledge of processes of erosion and transport of moraine by ice is still very limited and needs much improvement (see Reference BoultonBoulton, 1987)

Isostatic loading and unloading of ice sheets on the Earth's crust has provided a prime source of data on the elasticity of the lithosphere and of the viscosity of the layers beneath (Reference LliboutryLliboutry, 1971). A better appreciation of the mass of former ice sheets has significantly improved such calculations.

On a broader front, the study of the dynamics of polar ice sheets provides the largest-scale example of a material of known physical composition (ice plus around 0.01% by weight of air) whose physical properties determined in the laboratory can be related to the continental scale deformation of the same material on Earth. Although there are some basic differences with rock-forming minerals, many physical principles that have been shown to apply on ice sheets may well be applied to the solid Earth. Application of glaciologically derived concepts to studies of deformation of the Earth's mantle (Reference WeertmanWeertman, 1962) provide an example of such cross fertilization of ideas between solid Earth scientists and ice-sheet glaciologists.

Propagation of water-filled crevasses to the base of glaciers due to the greater density of water than ice has its counterpart in the upward opening of cracks in the Earth's crust due to the lower density of molten magma than the surrounding rock. Reference WeertmanWeertman (1971) has tackled both problems with the same theory.

Interaction between ice shelves and oceans is another field where data from radio-sounding of ice shelves (Reference RossRobin and others, 1983) and that from salinity-temperature-depth profiling of ocean waters (Reference Foldvik, Foldvik, Kvinge, Tørresen and JacobsFoldvik and others, 1985) provide complementary evidence about processes responsible for formation of the cold, dense Antarctic bottom water that spreads to beyond the Equator in the Atlantic Ocean.

These are a few examples that show the importance of the studies of ice sheets to our understanding of the planet on which we live – and even to that of any other planets with ice caps. Their value lies both in provision of data of global significance that cannot be found from any other source as well as their broader value in the study of the mechanics of deformation of vast, terrestrial solid masses such as the Earth's mantle.