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Longitudinal Stress Gradients and Basal Shear Stress of a Temperate Valley Glacier

Published online by Cambridge University Press:  30 January 2017

Robert Bindschadler*
Affiliation:
Geophysics Program AK-50, University of Washington, Seattle, Washington 98195, U.S.A.
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Abstract

For the first time field data from a temperate valley glacier, the Variegated Glacier, are used to investigate the behavior of longitudinal stress gradients predicted by the relation 1 where H is the local depth, and ys and yb are the surface and bed elevations respectively. This equation is similar to one derived by Budd (1970) for plane strain-rate, to evaluate the importance of longitudinal stress gradients, but a shape factor f is included to account approximately for lateral strain-rate gradients. Predictive numerical models of valley glaciers require the local base shear stress to be known as accurately as possible. It has been argued on theoretical grounds that when T is averaged over distances of more than five to ten times the depth, this term is negligible. At larger averaging scales, 2G can then be considered a correction to the simple geometric expression of base stress due to the presence of longitudinal stress gradients. Field data of velocity and geometry are used to evaluate the terms of Equation (1), where τb and 2G are estimated as and at intervals of 100 m, Us is the measured surface center-line velocity, A and n are the flow-law parameters, and is the surface longitudinal strain-rate. The expression for 2G is an approximation proposed by Budd (1970).

Type
Abstracts of Papers Presented at the Symposium but not Published in Full in this volume
Copyright
Copyright © International Glaciological Society 1979

The precise method of distance averaging is investigated carefully. Two methods are considered: a running arithmetic mean and a digital low-pass filter. By Fourier analysis the former method is converted to the form of a frequency operator for comparison with the latter. Because the magnitudes of 2G and T depend on the wavelength of the averaging scale, it is argued that for our case the digital low-pass filter is more appropriate. This method has the additional advantage that high-frequency noise in the data, predominantly a result of measurement errors, is more effectively removed.

Both operators are applied to the data to test the ability of 2G to correct τ g for averages of ¼, 1, 2, 4, and 10 km. The average depth of the glacier is 270 m, and T is neglected in all cases. Remnant high frequency in the data arithmetically averaged interferes with any attempt to judge the effectiveness of 2G as a correction. For no averaging length does the correction seem to be effective, although an averaging scale of 4 km appears to be the least poor. Comparison is easier with the frequency-filtered data. The agreement is best for the 4 km filter, where 2G accounts for a large fraction of the difference between τ b and τ g over most of the filtered region. However, for large-scale filters, most data are only partially filtered. For the 4 km filter, these edge effects eliminate 75% of the data field.

The conclusion is that in this analysis, 2G does not provide an effective means of improving the calculation of base shear stress on Variegated Glacier. This contrasts with the agreement found by Reference BuddBudd (1970) using Wilkes Ice Cap data. Possible explanations of this discrepancy include: errors in the field data or the shape factor may be too large to permit meaningful evaluation of a small correction term; T may be significant over some regions of this glacier; the relation used to evaluate 2G may be inappropriate for this valley glacier.

Discussion

W. F. Budd: Can you use your results to calculate an effective “viscosity” parameter for longitudinal stress ?

R. A. Bindschadler : Yes, I foresee no difficulty.

References

Budd, W. F. 1970. The longitudinal stress and strain-rate gradients in ice masses. Journal of Glaciology, Vol. 9, No. 55, p. 1927.CrossRefGoogle Scholar