Theory of Performance of Isothermal Solid-Nose Hotpoints Boring in Temperate Ice

Abstract The performance of a thermal ice-drill having a smooth, solid, impervious frontal surface, termed a “solid-nose hotpoint”, is determined by the velocities, pressures, and temperatures in the thin layer of warm melt water between the hotpoint and the ice. The efficiency, the speed of penetra...

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Published in:Journal of Glaciology
Main Author: Shreve, R. L.
Format: Article in Journal/Newspaper
Language:English
Published: Cambridge University Press (CUP) 1962
Subjects:
Online Access:http://dx.doi.org/10.1017/s0022143000027362
https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022143000027362
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spelling crcambridgeupr:10.1017/s0022143000027362 2024-04-28T08:26:45+00:00 Theory of Performance of Isothermal Solid-Nose Hotpoints Boring in Temperate Ice Shreve, R. L. 1962 http://dx.doi.org/10.1017/s0022143000027362 https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022143000027362 en eng Cambridge University Press (CUP) Journal of Glaciology volume 4, issue 32, page 151-160 ISSN 0022-1430 1727-5652 Earth-Surface Processes journal-article 1962 crcambridgeupr https://doi.org/10.1017/s0022143000027362 2024-04-09T06:56:15Z Abstract The performance of a thermal ice-drill having a smooth, solid, impervious frontal surface, termed a “solid-nose hotpoint”, is determined by the velocities, pressures, and temperatures in the thin layer of warm melt water between the hotpoint and the ice. The efficiency, the speed of penetration, the temperature of the frontal surface, and the distribution of pressure on it can be calculated from the equations of non-turbulent fluid flow. For hotpoints whose frontal surfaces are isothermal and axially symmetric, these quantities are functions of the total input of power Q of the weight W on the hotpoint, of the radius a and “shape factor” S of the frontal surface, and of the pertinent physical properties of water and ice. The calculation shows that with increasing “performance number” the efficiency E decreases and the surface temperature θ 0 increases. Thus, for example, E = 1·00 and θ 0 = 0°C. when N = 0.0 E = 0·76 and θ 0 = 48°C when N = 1.4; and E = 0·60 and θ 0 = 103°C. when N = 3.0. The coefficient Λ is a constant equal to . The shape factor S is a dimensionless number between 0 and 1 that varies according to the shape of the frontal surface, greater values of S being associated with blunter profiles (thus S = 1.0 for a plane frontal surface perpendicular to the axis). For coring hotpoints the same numerical results are obtained, but the performance number is given by where 2 ϖ i a is the inside diameter of the hotpoint. Article in Journal/Newspaper Journal of Glaciology Cambridge University Press Journal of Glaciology 4 32 151 160
institution Open Polar
collection Cambridge University Press
op_collection_id crcambridgeupr
language English
topic Earth-Surface Processes
spellingShingle Earth-Surface Processes
Shreve, R. L.
Theory of Performance of Isothermal Solid-Nose Hotpoints Boring in Temperate Ice
topic_facet Earth-Surface Processes
description Abstract The performance of a thermal ice-drill having a smooth, solid, impervious frontal surface, termed a “solid-nose hotpoint”, is determined by the velocities, pressures, and temperatures in the thin layer of warm melt water between the hotpoint and the ice. The efficiency, the speed of penetration, the temperature of the frontal surface, and the distribution of pressure on it can be calculated from the equations of non-turbulent fluid flow. For hotpoints whose frontal surfaces are isothermal and axially symmetric, these quantities are functions of the total input of power Q of the weight W on the hotpoint, of the radius a and “shape factor” S of the frontal surface, and of the pertinent physical properties of water and ice. The calculation shows that with increasing “performance number” the efficiency E decreases and the surface temperature θ 0 increases. Thus, for example, E = 1·00 and θ 0 = 0°C. when N = 0.0 E = 0·76 and θ 0 = 48°C when N = 1.4; and E = 0·60 and θ 0 = 103°C. when N = 3.0. The coefficient Λ is a constant equal to . The shape factor S is a dimensionless number between 0 and 1 that varies according to the shape of the frontal surface, greater values of S being associated with blunter profiles (thus S = 1.0 for a plane frontal surface perpendicular to the axis). For coring hotpoints the same numerical results are obtained, but the performance number is given by where 2 ϖ i a is the inside diameter of the hotpoint.
format Article in Journal/Newspaper
author Shreve, R. L.
author_facet Shreve, R. L.
author_sort Shreve, R. L.
title Theory of Performance of Isothermal Solid-Nose Hotpoints Boring in Temperate Ice
title_short Theory of Performance of Isothermal Solid-Nose Hotpoints Boring in Temperate Ice
title_full Theory of Performance of Isothermal Solid-Nose Hotpoints Boring in Temperate Ice
title_fullStr Theory of Performance of Isothermal Solid-Nose Hotpoints Boring in Temperate Ice
title_full_unstemmed Theory of Performance of Isothermal Solid-Nose Hotpoints Boring in Temperate Ice
title_sort theory of performance of isothermal solid-nose hotpoints boring in temperate ice
publisher Cambridge University Press (CUP)
publishDate 1962
url http://dx.doi.org/10.1017/s0022143000027362
https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0022143000027362
genre Journal of Glaciology
genre_facet Journal of Glaciology
op_source Journal of Glaciology
volume 4, issue 32, page 151-160
ISSN 0022-1430 1727-5652
op_doi https://doi.org/10.1017/s0022143000027362
container_title Journal of Glaciology
container_volume 4
container_issue 32
container_start_page 151
op_container_end_page 160
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