Introduction
This paper presents measurements and observations on the glaciers that form the headwaters of Susitna River, located in central Alaska, U.S.A. (Fig. 1). Susitna River, the sixth largest in Alaska, drains a significant part of the south side of the Alaska Range. The study described here began as part of a proposed hydro-electric development project in the Susitna River basin (Reference Harrison, Drage, Bredthauer, Johnson, Schoch and FollcttHarrison and others, 1983). The original purpose of the study was to determine how the glaciers within the basin affect run-off and sediment supply in Susitna River (Reference Clarke, Johnson, Harrison and DwightClarke and others, 1985,1986; Reference ClarkeClarke, 1986). (For economic reasons, the hydro-electric project never progressed beyond the planning stages.)
Five large glaciers and 50 or 60 small glaciers form the headwaters of Susitna River. The five major glaciers are Susitna, West Fork, “East Fork”, Maclaren and Eureka Glaciers (Fig. 1). Maclaren and Eureka Glaciers feed the tributary Maclaren River. This paper focuses on the dynamics of Susitna Glacier and its tributaries, West Fork and East Fork Glaciers. Measured ice flux is compared to balance flux, and the equilibrium between the two (or the lack thereof) is taken to be an indicator of surge behavior. Supporting evidence for this interpretation of the flux comparison is provided by an evaluation of moraine patterns on pre- and post-surge aerial photographs of Susitna Glacier, and from a comparison of surface-elevation changes on the glacier since its last surge. The periodicity of glacier surges in the basin is also estimated.
As stated above, some glaciers in the area are surge-type. Prior work on glacier surges includes a summary of the variability and periodic nature of surges by Reference Meier and PostMeier and Post (1969). The studies of (Reference Dolgushin and OsipovaDolgushin and Osipova 1973,1978) on Medvezhy Glacier, of Reference Krenke and RototayevKrenkc and Rototacv (1973) on Kolka Glacier, and of Reference Clarke, Collins and ThompsonClarke and others (1984) on Trapridge Glacier have improved our understanding of glacier surges. Detailed observations on Variegated Glacier before, during and after its 1982– 83 surge have lent insight into the evolution of glacier geometry during a surge cycle (Reference Raymond and HarrisonRaymond and Harrison, 1988) and the mechanisms that lead to and maintain rapid glacier motion during a surge (Reference KambKamb and others, 1985). And, most recently, observations of the 1986–87 surge of Peters Glacier (Reference Echelmcyer, Buttcrfield and CuillardEchelmcyer and others, 1987) and the 1987–88 surge of West Fork Glacier (Reference Echelmeyer and HarrisonEchelmcyer and Harrison, 1989) have shown some of the similarities and differences between surges on different glaciers.
While these studies have led to significant developments in the understanding of glacier surges, there remain relatively few direct measurements on surge-type glaciers. The intent of this paper is to provide further information and understanding of this aspect of glacier dynamics and glacier dynamics in general. A brief discussion of previous work in the Susitna Glacier basin and
Glacier location map. The three tributaries of Susitna Glacier under discussion are labeled accordingly. Balance flux and actual flux are. estimated at the constrictions marked, by the black transverse bars. Asterisks denote accumulation- and ablation-stake locations. The transverse bars cover the points inhere velocity was measured. The dashed line denotes drainage divides. The cross-section on West Fork Glacier where depth has been measured is marked by a row of Xs.
a history of glacier surges in the basin opens the discussion.
Previous Work And Surge History
Susitna Glacier is roughly 35 km long and covers about 230 km2. It is a geometrically complex glacier (Fig. 1) and is well known to be of surge-type (Reference PostPost, 1960, Reference Post1969). Reference PostPost (1960) estimated that the last surge occurred in 1952 or 1953 with ice displacements of about 4 km. Post estimated the displacements from oblique aerial photographs taken in 1942 (B. Washburn; Boston Museum of Science) and U.S. Geological Survey (USGS) vertical aerial photographs taken in July 1954. Since the study of Reference PostPost (1960), other aerial photographs have been located. Photographs taken on 29 August 1949 (USGS) show no signs of surging, and photographs taken on 5 July 1952 (USGS) show the surge front about 400 m from its July 1954 position. With these further time constraints, it appears that the surge had nearly ended by mid-summer 1952 and was initiated no earlier than winter 1949–50. The surge propagated a considerable distance into previously stagnant ice, but stopped 2 km short of an earlier surge. No other historical observations of Susitna Glacier prior to 1942 are known to exist, and the glacier has not surged since 1952.
West Fork Glacier, 40 km long and covering about 257km2, was first identified as surge-type by Reference PostPost (1969). This glacier is perhaps less known as surge type but has, in fact, just ended a spectacular surge. Hints of an impending surge were first noticed by A. Post and B. Krimmel during a photographic flight in late August 1987 (Post, USGS internal memorandum, 1988). In early January of the following year, Reference Echelmeyer and HarrisonEchelmeyer and Harrison (1989) noticed extensive shearing along the glacier margins. By February they found the glacier was clearly undergoing a strong surge with draw-down having propagated far into the accumulation area, and previously stagnant ice was being activated by a well-defined surge front. In total, when the surge terminated in early July 1988, about 35 km of the glacier length had been activated. A detailed study of this surge (personal communication from W. Harrison and K. Echelmeyer) and its effects on the sediment budget of Susitna River (personal communication from C. Raymond, R. Benedict and E. Chaco) is currently in progress. Post (written communication to S. C. Wilbur, 1984) estimated the previous surge of West Fork Glacier to have occurred in approximately 1937. This was estimated from oblique aerial photographs taken by B. Washburn in July 1940. Judging from the extremely crcvassed nature of the present glacier surface (2 years after surge termination) and the comparatively smooth “healed” surface depicted in the 1940 photographs, Post’s assessment that a surge had occurred 3 years prior to 1940 may be an underestimate. It appears more likely that the surge had occurred perhaps 5 years prior to 1940, placing it in roughly 1935 rather than 1937.
No other photographic information prior to 1940 is known to exist on West Fork Glacier except for a few ground photographs taken in August 1913 by the F. H. Moffit (USGS) railroad survey parties. These photographs show no evidence of active surge. However, a careful examination of color infrared stereo photographs taken by the National Aeronatics and Space Administration (NASA) in 1980 reveals three successively younger and less extended surge terminal positions (Fig. 2). About 0.5 km separates each terminal position. Pro-gressing upvalley, each terminal moraine (and the ground behind it) shows an essentially uniform stability and age of vegetation. Since there is no evidence of active surge on any photographs taken since 1940 (USGS, 1949, 1954, 1963, 1971, 1980), the least-extended and least-vegetated of these termini can be identified as a remnant of the 1935(?) surge. The 1987–88 surge fell about 1.1 km short of this most recent moraine.
Terminal moraine positions of West Fork Glacier. The ages of the. two most extended surge positions could not be determined. The westernmost channel depicted here was the primar-y drainage prior to, during and after the 1981–88 surge. (From 1980 NASA and 1989 University of Alaska photographs.)
East Fork Glacier is smaller and geometrically simpler than either Susitna or West Fork Glaciers. It is about 18 km long and covers 42 km2. East Fork Glacier has been examined by several authors, each of whom concluded that it is not a surge-type glacier. Reference PostPost (1969) determined this from the examination of historical aerial photographs and many years of observations. Harrison and R & M Consultants (1982) concluded this after comparing the 1949–80 displacement of a distinct marker on the glacier surface (a rock slide) to the glacier center-line velocity surveyed in late summer 1982. The 1949–80 displacement was measured from aerial photographs. The surveyed velocity fell within 1% of the average 1949–80 velocity, and from this they concluded it was unlikely that a major surge took place between 1949 and 1980. Reference WilburWilbur (1988) also concluded this after an extensive examination and comparison of hundreds of aerial photographs in the USGS photographic libraries. Using the designations set forth in the Canadian Glacier Inventory (Reference OmmanneyOmmanney, 1980), Wilbur assigned East Fork Glacier a surge code of 1 on a 0 to 5 point scale. (The Canadian Glacier Inventory assigns 0 to a glacier with no special surge features and assigns 5 to a glacier that is certain to be of surge type (Reference Clarke, Schmok, Ommanncy and CollinsG. K. C. Clarke and others, 1986). In the same work, for comparison, West Fork Glacier was assigned a code of 4 and Susitna Glacier a code of 5.
Eureka and Maclaren Glaciers are similar to East Fork Glacier in size and complexity. Eureka Glacier is about 11 km long and covers 39 km2; Maclaren Glacier is about 19 km long and covers 59 km2. Less is known of the history of these two glaciers. Eureka Glacier is listed as surge type and Maclaren Glacier is listed as inconclusive by Reference PostPost (1969). Reference MayoMayo (1978) noted that Maclaren Glacier underwent a weak surge or strong “pulse” in 1971. A mid- to late-summer ground-based photograph of Maclaren Glacier taken by Moffit (USGS) in 1910 or 1911 shows what appears to be fresh crevassing in the terminal area, but the photograph is very low angle, making it difficult to interpret definitively. Reference WilburWilbur (1988) assigned a Canadian Glacier Inventory code of 2 to Eureka Glacier and a code of 3 to Maclaren Glacier.
Methods
Field measurements for this project were undertaken during the 1981, 1982 and 1983 field seasons. Stakes were drilled into the glacier surfaces at approximately 1100, 1500 and 2000 m elevations to monitor point balance and velocity. One stake was maintained at each of these elevations on both West Fork and East Fork Glaciers. Susitna Glacier was studied somewhat more intensively because of its known surge history, and because of its complexity. Each of its three tributaries was monitored individually with separate 1500 and 2000 m elevation stakes for each. The tributaries share a common ablation area and therefore had a common 1100 m elevation stake. Velocity was measured at the mid-elevation stakes only. Also, the mid-elevation stakes were located at valley constrictions (Fig. 1) which enabled ice flow through a simple cross-section to be estimated. The constrictions were chosen as close to the equilibrium lines as possible (usually about 150–200 m below the average equilibrium-line altitude), so balance flux through the cross-section would be a maximum. In 1982, helicopter altimetry was used to record glacier-surface elevation near several of the stakes. Elevations were measured in mid-May and on 20 September. The altimeter was calibrated on points of known elevation during the surveys. Owing to logistical difficulties, velocity information was not collected on Maclaren or Eureka Glaciers.
Glacier velocity
Glacier center-line velocity was measured at the mid-elevation markers by theodolite resection, and by time-lapse photography for a brief interval on East Fork Glacier as described by Reference Harrison, Raymond and MacKeithHarrison and others (1986a). Surveys at the beginning and end of the melt season provided winter and summer velocities, and mid-summer surveys provided velocity fluctuations during the melt season. Velocities derived from these surveys arc shown in Figure 3; those from the time-lapse photography (Reference Harrison, Raymond, Moore, Senear and MacKeithHarrison and others, 1986b) are given in Figure 4.
Figure 3 shows that the glaciers of the Susitna River basin, like many temperate glaciers, undergo significant seasonal velocity variations. Increases in velocity during
Glacier velocity versus time. (Modified from. Ha,rrison and R & M Consultants, 1982.)
the early part of the melt season caused up to a doubling of glacier velocity. A perhaps more interesting observation is that the lowest measured velocities on West Fork Glacier and two tributaries of Susitna Glacier occurred late in the melt season, rather than in the winter. The limited data in Figure 4 show that short-lived events of rapid motion also occur, as is common with other temperate glaciers (Reference IkenIken, 1978; Reference Iken, Röthlisberger, Flotron and HaeberliIken and others, 1983; Reference Harrison, Raymond and MacKeithHarrison and others, 1986a, Reference Harrison, Raymond, Moore, Senear and MacKeithb). The event in Figure 4 occurred late in the melt season against a background of slowly decreasing velocity.
The early melt-season velocity peak and late melt-season minimum have important implications for basal motion. Since the glaciers thin during the melt season
Velocity on East Fork Glacier as measured by time-lapse photography on a daily basis between Julian days 214 and 256 (1 August-12 September) 1982. A linear fit to the data, which are somewhat noisy, shows the trend prior to the motion event. (From Reference Harrison, Raymond, Moore, Senear and MacKeithHarrison and others, 1986b.)
(at least in the area where velocity was measured), the increase in speed during the early part of this season must be due to enhanced basal motion. This enhanced sliding is thought to be caused by increased meltwater input and storage within the glacier and at its bed (Reference HodgeHodge, 1974; Reference IkenIken, 1978, Reference Iken1981; Reference Iken, Röthlisberger, Flotron and HaeberliIken and others, 1983).
The late melt-season minimum is not as well known. The increased speed in winter cannot be explained by increased loading of the glaciers during winter. Average balance in the vicinity of the velocity stakes during the winter season (1 October-14 May) varied between +0.75 and +1.25 m ice equivalent, depending upon the glacier and year of measurement (Reference ClarkeClarke, 1986). This thickening is very small compared to the 400–700 m ice thicknesses at the velocity markers, and can at best only account for a few per cent of the winter-speed increase. This implies that, at least on the glaciers that show a velocity minimum in late summer, some of the winter motion is due to sliding. (It should be noted, however, that these seasonal velocity variations were only measured near (slightly below) the equilibrium lines on each glacier and may vary considerably elsewhere on each glacier.) Reference HodgeHodge (1974) observed a similar velocity minimum on Nisqually Glacier during the same season and, using essentially the same approach, found that changes in ice thickness could not explain its speed increase during winter. Rather, Hodge concluded that the only viable explanation for this speed-up was a steady increase in stored water at the glacier bed throughout the winter.
Comparison of balance flux to actual flux
We wish to compare mass balance above each velocity marker (balance flux) to ice flow (actual flux) at the respective velocity markers. For a glacier to be in flow equilibrium, the balance flux must equal the actual flux through the constrictions where velocity was measured. In order to determine the balance flux from measure-ments of accumulation, the time period over which mass balance is measured must be long enough to smooth out seasonal and annual variations in balance. Similarly, for an accurate determination of ice transport by glacier flow, the time period over which velocity is measured must be long enough to average out seasonal variations in velocity. In the discussion below, balance flux is estimated from 3 years of annual balance data, and actual flux is estimated from 2 years of velocity data.
Balance flux
The point-balance data collected from the stake network described above were used to construct annual balance versus elevation curves. Details of how these curves were constructed have been described by Reference ClarkeClarke (1986). The balance year was taken to be 1 October 30 September. Area elevation relations for each glacier were determined from 1:63 360 scale USGS topographic maps. Total annual balance above each velocity point for each year, Ba, could then be determined from the relation:
where bi is the annual balance per year in the ith elevation interval, ai is the area of the ith elevation element above the velocity gate, and m is the highest elevation element in the basin being considered. The results of these calculations are shown in Table 1.
Total annual ice balance above constrictions
As stated previously, total annual balance above a given cross-section, when averaged over several years, is approximately equal to balance flux. Unfortunately, the 1983 balances were not obtained for the northeast (locally referred to as “Turkey”) and northwest tributaries of Susitna Glacier because these accumulation-area stakes were buried by high snowfall that year. (This high snowfall is reflected in the balance data for the three glaciers that do have 1983 data.) If Table 1 is examined closely, it can be seen that the 1981 total annual balance is nearly equal to the 3 year average for West Fork and Susitna Glaciers’ cast tributary, which have complete 3 year data. The balance-flux estimates (shown in Figure 5) arc thus taken to be equal to the 1981 total annual balance for the northeast and northwest tributaries (which lie geographically between West Fork and the cast tributary); West Fork and Susitna Glaciers’ east tributary balance fluxes arc taken to be equal to the 3 year averages and, since there are no 1981 data for East Fork Glacier, its balance flux is taken to be the average of the 1982 and 1983 total annual balances.
Comparison of actual flux and balance flux.
Actual flux
Actual flux, Qa , can be approximated from the relation:
where us and ub are the surface and basal velocity at the center line, respectively; A is the cross-sectional area and S is a velocity shape factor. Channels were assumed to be parabolic with center-line depth h (determined below). The velocity shape factor was taken to be about 0.67 following Reference NyeNye (1965). In all cases, us was averaged over integral years as nearly as possible (2.04–2.08 a) to reduce errors in average speed due to seasonal variations. Dcformational velocity (us — ub ) was assumed to be equal to the lowest measured velocity on each glacier, and any increase in velocity over the lowest measured velocity was assumed to be caused by sliding. Velocity measurements from July 1981 to June 1983 were used in the calculation. The results of the actual flux estimates, shown in Figure 5, arc averages over this 1981–83 period.
Maximum glacier depth, h, was not measured during this study and therefore had to be approximated from the relation:
where n and A are flow-law parameters, set equal to 3 and 1.67 ×10−7 a−1 kPa−3, respectively (from Reference PatersonPaterson, 1981), f is the stress-shape factor (Reference NyeNye, 1965), ρ is ice density, g is the acceleration of gravity, and α is surface slope taken from USGS 1: 63 360 scale maps as averaged over about 15 ice thicknesses. The shape factor is dependent upon the ratio of width to depth, and depth is unknown, so the solution for f and h must be determined itcratively. The resulting values of f arc in the range of 0.50 0.57, with corresponding half-width to depth ratios varying from 1.23 to 1.52.
The parameter A was assumed to be that of temperate ice. A thermocouple string was placed 20 m deep high (2350 m elevation) on the northwest tributary of Susitna Glacier on 22 May 1981. By 3 August, the sensors showed isothermal conditions to at least this depth (Reference HarrisonHarrison, 1981). Given existing ideas on heat transfer in glaciers (e.g. Reference PatersonPaterson, 1981, chapter 10), it is reasonable to infer from this that the majority of the ice in the basin is temperate. Also, earlier work by Reference Harrison, Mayo, Trabant, Weiler and BowlingHarrison and others (1975) found nearby Black Rapids Glacier to be essentially temperate. Reference Harrison, Mayo, Trabant, Weiler and BowlingHarrison and others (1975) did, however, find a roughly 15 m thick —1°C to 2°C surface layer in the Black Rapids Glacier ablation area. These layers are common and are attributed to the inability of meltwater to percolate downward and rewarm the ablation area in spring (Reference PatersonPaterson, 1972). A similar cold layer probably also exists on the lower reaches of the Susitna basin glaciers but was not considered extensive enough to have a significant effect on flow. (Note that Black Rapids, Susitna and East Fork Glaciers all share the same ice field but flow in different directions (Fig 1.
Velocity data from East Fork Glacier were obtained in late summer only and arc insufficient to determine its pattern of seasonal velocity variation. For the purpose of calculating ice depth, East Fork Glacier was assumed to be similar to the surrounding glaciers, so the late summer velocity given in Figure 3 was taken to be entirely due to internal deformation, realizing that the actual pattern is complicated by the occurrence of short-period motion events (Fig. 4). Since it was also necessary to use this same velocity in the calculation of actual flux, the * Qa .and ub estimated from measured depth.
Estimated maximum ice thickness in cross-sections
Estimated actual ice flux per year through the cross-sections. Actual flux shown here is the July 1981-June 1983 yearly average
re-suiting flux would be a minimum since seasonal sliding had not been included. Flux due to sliding for the other four glaciers averaged about 22% of the total flux, so a similar adjustment was made to the East Fork Glacier result. The results of the depth calculations arc shown in Table 2, and the final actual flux estimates are shown in Table 3.
An independent check on the reliability of the depth estimates can be obtained by a comparison with a cross-section on West Fork Glacier where ice depth has recently been measured. The cross-section is located about 1 km down-glacier of the velocity measurement point (Fig. 1) and is approximately parabolic, as assumed in the calculations above. Ice depths, provided by B. Weert-man (written communication, 1990) were measured by radio-echo sounding. The measured maximum depth, 675 m, and calculated depth, 810 m, agree reasonably well (Table 2).
It should be noted that the actual flux results are relatively insensitive to the partitioning of the motion between deformation and sliding. This is because, for example, an underestimate of basal sliding lowers average sectional velocity (Equation (2)), but this also leads to an overestimate of internal deformation and therefore an overestimate of maximum glacier depth (Equation (3)). These two effects tend to cancel themselves (within 10%). West Fork Glacier serves as a good example. If West Fork Glacier’s flux is determined from the 675 m measured thickness and “true” sliding velocity (i.e. any velocity not explained by glacier thickness and slope), Qa = 56.0 × 106 m3 a−1 results. If the same calculation is performed using the 810 m calculated depth, and the assumed sliding velocity (i.e. any velocity over the minimum measured velocity, Qa = 56.0 × 106 m3 a−1results.
Discussion
The estimates of actual flux and balance flux arc compared in Figure 5. Table 4 shows the ratios of actual flux to balance flux. A ratio of 1.00 means the glacier is transporting its accumulated mass down-glacier each year. This is interpreted to mean that a particular glacier is not building a reservoir of ice which could, for example, be released during a surge. From Figure 5 it is clear that three of the five glaciers listed show a significant imbalance between actual fluxand balance flux. The cast tributary of Susitna Glacier shows the greatest discquilibrium with only about 24% of the accumulation being transported out of that basin. West Fork Glacier and the northeast tributary of Susitna Glacier show transports of 44% and 57%, respectively. The northwest tributary and East Fork Glacier show no discernible imbalance.
Ratio of actual flux to balance flux
Evolution of moraines on Susitna Glacier. Left and center are from Reference Meier and PostMeier and Post (1969). Note that the 1951–52 surge did not extend as far as the prior surge. (Modified from Reference Harrison, Drage, Bredthauer, Johnson, Schoch and FollcttHarrison and, others, 1983.)
It is important to realize that an inequality between balance flux and actual flux does not necessarily imply that a glacier is building toward a surge. Reference HolmlundHolmlund (1988), using a similar comparison on Storglaciären, Sweden, found that a disequilibrium occurred there because of changes in mass balance on the glacier. However, prior surge history and other evidence (discussed below) indicate that the imbalance measured here is more likely caused by a rebuilding between surges rather than a change in mass balance.
The ratios listed in Table 4 for Susitna Glacier apparently indicate that its northwest tributary contributes little to a surge; its cast tributary contributes significantly, and its northeast tributary apparently lies somewhere between these two. (It should be noted, however, that the disequilibrium of the northeast tributary is similar to that of West Fork Glacier which just underwent a strong surge.)
Other evidence for the relative surge strength of these tributaries can be found by examining moraine struc-tures in sequential aerial photographs. Figure 6 shows the evolution of moraine patterns from just before the 1951–52 surge to just after the surge and their appearance in 1980. In 1949, the moraines of the northwest tributary show it to be flowing vigorously into the relatively sluggish main trunk; this lobe was sheared off and carried down-glacier by the 1951–52 surge, and the lobe again grew steadily after the surge until at least 1980. Note that this tributary contributed little to the surge. The northeast tributary appears to show a similar vigorous flow prior to the surge. It did, however, contribute a significant amount of ice to the surge as is shown in the 1954 photograph (Fig. 6b). This reflects its intermediate surge character. The relatively stagnant east tributary became active only during surge, reflecting its strong surge character.
It is arguable that, if both the northeast and east tributaries show significant participation during a surge, then one tributary does not necessarily surge more strongly than the other. However, if one tributary lies nearly stagnant between surges, and the other continues to flow rather normally, then the two are different in their overall dynamics.
According to Figure 5 and Table 4, the accumulation area of Susitna Glacier’s east tributary should be thick-ening. As mentioned previously, glacier center-line surface elevation on this branch was measured in 1982. A comparison of the altimetry data and map-elevation data is shown in Figure 7. In the vicinity of the accumulation stake, this tributary did indeed thicken by approximately 60 m between 1956, when the glacier was mapped (written communication from M. Southern, 1984), and 1982. The question arises as to whether this rate of thickening is in agreement with the expected rate of thickening due to the inequality between actual flux and balance flux.
If the distribution of thickness change is integrated over the area of the glacier above the velocity marker (over only that area affected by the 1951–52 surge), an average ice-thickness change of +0.80 ± 0.32 m a−1 results for the 1956–82 period. This is to be compared with the +0.92 ± 0.44 m a−1 difference between balance flux and actual flux for the 1981–83 period in the same basin. Although the two rates of thickening are averages over different times in the surge cycle, the similarity between them shows the flux comparison to be reasonable.
The disequilibrium of West Fork Glacier is confirmed by its 1987–88 surge. If Figure 3 is examined, it is clear that West Fork Glacier’s velocity, excluding the spring speed-up period, increased substantially between 1981–82 and 1982–83. Since glacier slope and thickness did not change appreciably over this 1 year period, this 29% increase is very likely due to an increase in basal sliding. It is interesting that Variegated Glacier showed a very similar speed increase of about 26% annually, at a similar location on the glacier, during the 7 years prior to its 1982–83 surge (Reference Raymond and HarrisonRaymond and Harrison, 1988).
Surge Period
How often may surges be expected to occur in the Susitna River basin? West Fork Glacier surged in about 1935 and again in 1987–88, indicating a surge period of about 50–60 years. Based on the information discussed above, it appears likely that Susitna Glacier is also readying for another surge. Estimates of its surge period can be obtained in at least two ways, both of which are founded upon the non-surge behavior of the northwest tributary.
First, there is an icefall in the northwest tributary that produces ogives. Ogives are known to form on an annual basis (Reference NyeNye, 1958). By 1949, roughly 47 (±5) of these ogives had crossed from the tributary into the main glacier (USGS photograph, 1949). If it is assumed that, as in 1951–52, this lobe was sheared off and carried down-glacier by the surge prior to 1951–52, it appears that the new lobe had been forming for about 47 years by 1949. Since the glacier surged 2 or 3 years later, a period of about 50 years is indicated.
The second estimate can be obtained by simply comparing the area of this same lobe just before the 1951–52 surge to the area of the new lobe in 1980. The pre-surge lobe covered an area of 4.0 km2 in 1949. By 1980 the new lobe had grown to 2.0 km2. The ratio of these areas multiplied by the time it took the new lobe to grow to its 1980 size yields a similar surge period of roughly 56 years.
It is also reasonable that surge period and flux imbalance are related. Unfortunately, flux imbalance has large temporal and spatial dependences associated with it. For example, Reference Bindschadler, Harrison, Raymond and CrossonBindschadler and others (1977) found Variegated Glacier to have a flux imbalance (in the mid-1970s) of about 7:1, but by 1981 its imbalance had decreased to about 2.6:1, 1 year before the glacier surged (from Reference Raymond and HarrisonRaymond and Harrison, 1988). It seems then that a glacier’s flux imbalance can only be related to surge period if the variation in the imbalance is known over most of the quiescent phase. Also, the two fluxes must be compared near the lower reaches of the surge supply area (if the fluxes were compared above the supply area obviously no imbalance would be observed), and the approximate quantity of ice transferred down-glacier during a surge must be known. If these factors arc known, then the supply-area refill rate could be used to determine an approximate surge period. This is of course further complicated by the fact that the quantity of ice moved during different surges on the same glacier can vary considerably (e.g. Figs 2 and 6b).
Surface-elevation change, from. 1950 to 1982 on the center line of the east tributary of Susitna Glacier. Distance shown on the ab-scissa is distance from the head of the glacier.
Summary
Actual ice flux and balance flux have been compared on West Fork Glacier, East Fork Glacier and the three tributaries of Susitna Glacier. The comparison is a useful tool for determining the likelihood of surge behavior, and can be used to distinguish differences in dynamics of separate tributaries of the same glacier. The mass balance and velocity data used for this comparison are admittedly quite sparse, and have large errors associated with the parameters derived from them. However, when these data are viewed in combination with those taken from aerial photographs, moraines, maps and altimetry, a reasonably consistent picture develops: West Fork Glacier is a surge-type glacier and it may be expected to surge about every 50–60 years, as borne out by its recent behavior. The three tributaries of Susitna Glacier show markedly different dynamics. The northwest tributary shows little or no surge character; it flows normally and participates very little during surges. The east tributary exhibits a very strong surge character; it moves very slowly during the glacier’s quiescent phase and is very active during surge. The northwest tributary’s dynamics lie somewhere between these two; it flows rather vigorously during quiescence but also participates significantly during surge. Like West Fork Glacier, Susitna Glacier may also be expected to surge every 50–60 years. This places the next surge of Susitna Glacier in the first decade of the 21st century. East Fork Glacier is not a surge-type glacier, as was found by several earlier authors (Reference PostPost, 1969; Harrison and R & M Consultants, 1982; Reference WilburWilbur, 1988).
Seasonal velocity variations of these glaciers show several interesting features. Speed during early summer, at the resolution of these measurements, can be as much as double the winter speed. The annual velocity minimum on some glaciers occurs in late summer. This implies that these particular glaciers are sliding in winter. Moreover, although the data are limited, events of rapid motion, lasting a day or so, also occur. Finally, West Fork Glacier showed a 29% increase in speed over the 2 year period of measurement. This speed increase was measured 5 years prior to its most recent surge and is similar to Variegated Glacier’s annual speed increases over several years prior to its surge (Reference Raymond and HarrisonRaymond and Harrison, 1988).
Acknowledgements
The author would like to express his sincere gratitude to W. Harrison and K. Echelmcyer for their discussions, perspective and encouragement during the preparation of this manuscript, and for the comments provided by an anonymous reviewer. The excellent work of D. Johnson and C. Moore in the field provided most of the quantity and quality data that were available to work with. C. Schoch of R & M Consultants also contributed greatly to the field efforts. Co-operating companies or agencies have been R & M Consultants of Anchorage, Alaska, Acres American, Inc., Harza Ebasco Susitna Joint Venture, the Alaska Power Authority and the State of Alaska Division of Geological and Geophysical Surveys. Financial support has been from the Alaska Power Authority, the State of Alaska Division of Geological and Geophysical Surveys, the University of Alaska and the U.S. National Science Foundation, Division of Polar Programs. The preparation of this manuscript was made possible under U.S. NSF grant numbers DPP-8822624 and DPP-8519110.
