Introduction

The 1965-66 surge of Steele Glacier, Yukon Territory, Canada, is one of the best documented surge advances of a large glacier. Field work by Reference WoodWood (1936,1942) and Reference SharpSharp (1943,1951) provided much information about the pre-surge condition of the glacier, and the onset of the surge phase was detected by A. S. Post in the fall of 1965. Although there is an unfortunate gap in information for the period between Post’s surge prediction and the peak of surge activity in mid-1966, a number of useful observations were made during the decline of the surge phase (Reference BayrockBayrock, 1967;Reference Stanley Stanley, 1969; Reference Thompson, Bushnell and RagleThomson, 1972).

Prior to July 1972 geophysical measurements on Steele Glacier were lacking, but investigations of two small surge-type glaciers near the Steele gave a consistent picture of the relationship between ice temperature and depth for pre-surge glaciers in the region: both glaciers were cold with large regions of temperate or near-temperate basal ice. This evidence was taken as support for thermal control of the surges. Although the Steele is much larger than the two glaciers studied previously, it seems reasonable that all of the eighteen probably surge-type glaciers of the Steele Creek basin surge by the same mechanism. Results of the 1972 reconnaissance drilling program on Steele Glacier (Reference Jarvis and Clarke Jarvis and Clarke, 1974) left the question of the Steele’s surge mechanism unsettled, but did indicate that the 1965-66 surge had greatly disturbed the thermal regime in the middle zone of the glacier.

Deep drilling at three additional sites in 1973 and subsequent ice temperature measurements taken in 1974 provide further evidence of anomalous temperatures. The four deep-drilling sites, all located below the firn line, are indicated in Figure 1. Surging of tributary glaciers such as the Hodgson Glacier and several unnamed glaciers leads to some confusion as to what ice is original to the Steele Glacier and what flows from tributaries. Medial moraines allowed the ice origin to be traced and it is thought that all drilling sites were located on ice flowing from either of the two main arms of the Steele. Drilling sites 73-2 and 73-3 were located in a region which prior to the last surge was covered by stagnant debris-laden ice; sites 72-1 and 73-1 were in the zone which remains active during the quiescent phase. All sites except 73-3 were in severely crevassed regions of extending flow during most of the surge.

Fig. 1. Locations of 1972 and 1973 thermal drilling sites on Steele Glacier.

Measurements And Results

Holes were thermally drilled using several different modifications ofReference Aamot Aamot’s (1968) buoyancy-stabilized probes. From past experience we found that buoyancy chambers reduced thermal contact and hence drilling rate; this disadvantage more than outweighed the merits of self-steering so the air chambers were filled with epoxy resin. Glass-beaded thermistors calibrated in the laboratory to an accuracy of ±0.04 deg were connected to 8-conductor cable and allowed to follow the thermal probe through the ice. No attempt was made to recover the probes. More complete details of probe design, thermistor calibration and field procedures are given elsewhere (Reference Classen, Clarke, Bushnell and RagleClassen and Clarke, 1972; Reference JarvisJarvis, unpublished).

Thermistor resistances were measured in September 1974, more than one year after completion of thermal drilling. A Fluke 8 100A digital multimeter and a Danameter 2000 were used to make these measurements to a final accuracy of ± 0.075 deg.

Table 1 lists the observed ice temperatures with depth at the four sites, together with the dates of drilling and temperature measurement. The codes 72T to, 72 l11, etc., label thermistor cables. Temperatures indicated as greater than 0.00°C were for thermistors which had melted out of the ice and were lying on the glacier surface. The temperature profile for site 72-1 (referred to the 1972 ice surface) is presented as Figure 2. The anomalous reversed temperature gradient between 45 m and 115 m is probably due to water injection into crevasses formed during the surge. A theoretical temperature curve for the effect of a spatially periodic field of partially water-filled crevasses on ice temperature agrees well with observations. The holes drilled at site 73-1 above the confluence of the Hodgson Glacier show a similar inversion which can also be accounted for in this way (Fig. 3). The input parameters for the crevasse models used in generating the theoretical curves in Figures 2 and 3 are given

Fig. 2. Measured ice temperature with depth in hole at site 72-1. The smooth curve is the predicted temperature with depth at a time 7.5 years after the surge onset assuming a spatially periodic field of partially water-filled crevasses was formed during the surge.

Fig. 3. Measured ice temperature with depth in holes at site 73-1 near the confluence with Hodgson Glacier. The smooth curve 15 the predicted temperature with depth at a time 8.5 years after the surge onset assuming a spatially periodic field of partially water-filled crevasses was formed during the surge.

in Table II; details of the numerical model have been published previously (Reference Jarvis and ClarkeJarvis and Clarke, 1974). Because final temperatures at sites 72-1 and 73-1 were not measured in the same summer field season, the theoretical curves plotted in Figures 2 and 3 are evaluated at times appropriate to each set of measurements.

A second type of anomalous profile was measured at site 73-2 near the "big bend" in Steele Glacier 15 km below the confluence with Hodgson Glacier (Fig. 4). The nearly isothermal temperature distribution cannot be an equilibrium feature and probably is the result of extreme water penetration through a relatively thick (100-200 m) layer of fractured ice. The profile labelled 73T7 was measured in a hole located approximately 7° 111 from the other holes at this site and at a distance of 20 m from an active moulin. It is interesting that this moulin exists in non-temperate ice and illustrates that internal drainage is not a feature unique to temperate glaciers.

The only temperature profile which could be characterized as "normal" was measured at site 73-3 in the moraine-covered stagnant ice near (he snout (Fig. 5). In this case the temperature increases regularly with depth and attains the melting point at approximately 85 m. Similar profiles have been observed on the nearby Rusty and Trapridge Glaciers

Fig. 4. Measured ice temperature with depth in holes drilled at site 73-2 near the "big bend" of Steele Glacier. The shallow hole 73T7 was drilled 20 m from a moulin and is located approximately 70 m from the remaining holes at this site.

(Reference Clarke and GoodmanClarke and Goodman, 1975; Reference Jarvis and ClarkeJarvis and Clarke, 1975). No soundings have been attempted on the Steele so it is not certain whether a thick layer of temperate ice lies below site 73-3 or whether the probe reached the bed. The slope discontinuity in temperature near 50 m is too large to be due to poor calibration or resistance measurement. At this site all thermistors were measured at least six times using two different meters; calibration accuracy for all thermistors at this site was better than 0.015 deg. As numerical modelling experiments (Reference ClarkeClarke, 1976) predict temperature kinks near the snout of a cold glacier that has recently surged, the feature is probably real. The lifetime of the present thermal anomaly at site 73-3 is less than ten years.

Fig. 5. Measured ice temperature with depth at site 73-3 3.3 km from the 1973 terminus.

With three of the four temperature profiles clearly "anomalous" it is premature to make generalizations concerning Steele Glacier’s thermal regime. Water penetration has greatly disturbed the temperature of the near-surface ice and our measurements were not sufficiently deep to allow prediction of the deep regime. We conclude that surging glaciers can have a very complex thermal structure which would not necessarily be revealed by shallow temperature measurements at a small number of sites. It is possible that some of these glaciers which have been identified as temperate from near-surface temperature may, in part, be sub-polar.

Acknowledgements

We thank Environment Canada, the University of British Columbia Committee on Arctic and Alpine Research, and the National Research Council (Canada) for financial support, and the Arctic Institute of North America for logistic support in the field. B. Chandra, D. F. Classen, B. B. Narod and K. D. Schreiber assisted with field preparations and R. Metcalfe was a congenial and capable field assistant. The co-operation of the National Parks Service, Kluane National Park, is gratefully acknowledged.

Discussion

G. DE Q. ROBIN: How long will it take for the water body in the crevasse to freeze completely? Could the anomaly at your lowest station be due to a very old water pocket that has been carried down?

G. K. C. CLARKE: Neither of the two crevasse models presented was run until the water pockets froze solid, but I would guess that complete freezing should occur 20-30 years after the time of the surge. It is certainly possible that thermal anomalies of the sort we observe do not disappear completely during the quiescent phase so that when the next Steele surge occurs the temperature will still be disturbed from the 1965-G6 surge. I agree that the anomaly at Site 73-3 could be caused in this way. We have computed several models in which we have two different crevasse-opening events, i.e. surges, but do not allow for ablation at the glacier surface, which must have a significant influence.

W. S. 13. PATERSON: I note that you regarded crevasse depth as a variable parameter. Have you made any measurements?

CLARKE: There are no longer any open crevasses near our drilling sites so we could not make this measurement.

J. W. GLEN: Most studies of crevasse depths are based on normal, slow glaciers. In a surging glacier, especially with good water supply, I do not see why any depth is unthinkable.

C. F. RAYMOND: DO you think penetration of water into moulins during the quiescent phase of flow represents a significant heal transport mechanism, which needs to be considered in calculating the evolution of temperature between surges?

CLARKE: I find it hard to imagine that a significantly dense network of drainage channels exists within the glacier to cause a major thermal disturbance.

M. F. MEIER: In July of 1966 one could see water in many crevasses, in some cases right next to crevasses which were completely dry. If one assumes that water is getting into all crevasses, then one must surmise that it also can escape from some. Perhaps the water escapes because these crevasses are very deep.