The Flow of a Glacier in a Channel of Rectangular, Elliptic or Parabolic Cross-Section

Abstract Numerical solutions are found for the steady rectilinear flow of ice, obeying Glen’s non-linear flow law, down uniform cylindrical channels of rectangular, semi-elliptic and parabolic cross-section. The results are also directly applicable to the pumping of a non-Newtonian fluid down a pipe...

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Published in:Journal of Glaciology
Main Author: Nye, J. F.
Format: Article in Journal/Newspaper
Language:English
Published: Cambridge University Press (CUP) 1965
Subjects:
Online Access:http://dx.doi.org/10.1017/s0022143000018670
https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022143000018670
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spelling crcambridgeupr:10.1017/s0022143000018670 2024-09-15T18:15:39+00:00 The Flow of a Glacier in a Channel of Rectangular, Elliptic or Parabolic Cross-Section Nye, J. F. 1965 http://dx.doi.org/10.1017/s0022143000018670 https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022143000018670 en eng Cambridge University Press (CUP) Journal of Glaciology volume 5, issue 41, page 661-690 ISSN 0022-1430 1727-5652 journal-article 1965 crcambridgeupr https://doi.org/10.1017/s0022143000018670 2024-08-28T04:02:57Z Abstract Numerical solutions are found for the steady rectilinear flow of ice, obeying Glen’s non-linear flow law, down uniform cylindrical channels of rectangular, semi-elliptic and parabolic cross-section. The results are also directly applicable to the pumping of a non-Newtonian fluid down a pipe. There is assumed to be no slip of the ice on the channel surface. Certain results on the centre-line velocity in symmetrical channels may be derived purely from dimensional and symmetry principles. An analytical solution due to Dr. W. Chester is given for a semi-elliptic channel section which departs only slightly from a semi-circle. Contrary to a view sometimes held, the maximum shear stress at the ice surface in a parabolic channel and in some elliptical channels does not always occur at the edge. With the flow law, strain-rate proportional to (stress) 3 , the velocity averaged across the ice surface, which is easily measured with a line of stakes, is close to the average velocity over the whole section for a wide range of parabolic sections; the hydrological importance of this result is that the discharge may be inferred without the need to measure the velocity at depth. Arguments are given to show that the result still holds when there is slipping on the bed and when the power in the flow law differs somewhat from 3, Depending on the amount of bed slip and the shape of the channel section, the kinematic wave velocity for a range of parabolic channels is between 2.0 and 2.3 times the centre-line velocity of the ice, and between 2.0 and 3.5 times the mean surface velocity of the ice. Article in Journal/Newspaper Journal of Glaciology Cambridge University Press Journal of Glaciology 5 41 661 690
institution Open Polar
collection Cambridge University Press
op_collection_id crcambridgeupr
language English
description Abstract Numerical solutions are found for the steady rectilinear flow of ice, obeying Glen’s non-linear flow law, down uniform cylindrical channels of rectangular, semi-elliptic and parabolic cross-section. The results are also directly applicable to the pumping of a non-Newtonian fluid down a pipe. There is assumed to be no slip of the ice on the channel surface. Certain results on the centre-line velocity in symmetrical channels may be derived purely from dimensional and symmetry principles. An analytical solution due to Dr. W. Chester is given for a semi-elliptic channel section which departs only slightly from a semi-circle. Contrary to a view sometimes held, the maximum shear stress at the ice surface in a parabolic channel and in some elliptical channels does not always occur at the edge. With the flow law, strain-rate proportional to (stress) 3 , the velocity averaged across the ice surface, which is easily measured with a line of stakes, is close to the average velocity over the whole section for a wide range of parabolic sections; the hydrological importance of this result is that the discharge may be inferred without the need to measure the velocity at depth. Arguments are given to show that the result still holds when there is slipping on the bed and when the power in the flow law differs somewhat from 3, Depending on the amount of bed slip and the shape of the channel section, the kinematic wave velocity for a range of parabolic channels is between 2.0 and 2.3 times the centre-line velocity of the ice, and between 2.0 and 3.5 times the mean surface velocity of the ice.
format Article in Journal/Newspaper
author Nye, J. F.
spellingShingle Nye, J. F.
The Flow of a Glacier in a Channel of Rectangular, Elliptic or Parabolic Cross-Section
author_facet Nye, J. F.
author_sort Nye, J. F.
title The Flow of a Glacier in a Channel of Rectangular, Elliptic or Parabolic Cross-Section
title_short The Flow of a Glacier in a Channel of Rectangular, Elliptic or Parabolic Cross-Section
title_full The Flow of a Glacier in a Channel of Rectangular, Elliptic or Parabolic Cross-Section
title_fullStr The Flow of a Glacier in a Channel of Rectangular, Elliptic or Parabolic Cross-Section
title_full_unstemmed The Flow of a Glacier in a Channel of Rectangular, Elliptic or Parabolic Cross-Section
title_sort flow of a glacier in a channel of rectangular, elliptic or parabolic cross-section
publisher Cambridge University Press (CUP)
publishDate 1965
url http://dx.doi.org/10.1017/s0022143000018670
https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022143000018670
genre Journal of Glaciology
genre_facet Journal of Glaciology
op_source Journal of Glaciology
volume 5, issue 41, page 661-690
ISSN 0022-1430 1727-5652
op_doi https://doi.org/10.1017/s0022143000018670
container_title Journal of Glaciology
container_volume 5
container_issue 41
container_start_page 661
op_container_end_page 690
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