Comment on “Channel flow, tectonic overpressure, and exhumation of high-pressure rocks in the Greater Himalayas” by Marques et al. (2018)

<p>The upward-tapering channel model proposed by Marques et al. (2018) for the Himalayas has a “base” that forms part of the subducting footwall and therefore does not close the channel. This configuration does not produce return flow, and no dynamic overpressure develops in the channel. The g...

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Main Author: J. P. Platt
Format: Article
Language:English
Published: Copernicus Publications 2019-02-01
Series:Solid Earth
Online Access:https://www.solid-earth.net/10/357/2019/se-10-357-2019.pdf
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spelling doaj-4f71c1c485904a8ebdf57617675cc3292020-11-25T01:29:49ZengCopernicus PublicationsSolid Earth1869-95101869-95292019-02-011035736110.5194/se-10-357-2019Comment on “Channel flow, tectonic overpressure, and exhumation of high-pressure rocks in the Greater Himalayas” by Marques et al. (2018)J. P. Platt<p>The upward-tapering channel model proposed by Marques et al. (2018) for the Himalayas has a “base” that forms part of the subducting footwall and therefore does not close the channel. This configuration does not produce return flow, and no dynamic overpressure develops in the channel. The geometrical and kinematic configuration they actually use for their calculations differs from this and is both geologically and mechanically improbable. In addition, the fixed upper boundary condition in their models is mechanically unrealistic and inconsistent with geological and geophysical constraints from the Himalayan orogen. In reality, the dynamic pressures calculated from their model, which exceed lithostatic pressure by as much as 1.5&thinsp;GPa, would cause elastic flexure or permanent deformation of the upper plate. I estimate that a flexural upwarp of 50&thinsp;km of the upper plate would be required to balance forces, which would lead to geologically unrealistic topographic and gravity anomalies. The magnitude of the dynamic overpressure that could be confined is in fact limited by the shear strength of the upper plate in the Himalayas, which is likely to be &lt;&thinsp;120&thinsp;MPa.</p>https://www.solid-earth.net/10/357/2019/se-10-357-2019.pdf
collection DOAJ
language English
format Article
sources DOAJ
author J. P. Platt
spellingShingle J. P. Platt
Comment on “Channel flow, tectonic overpressure, and exhumation of high-pressure rocks in the Greater Himalayas” by Marques et al. (2018)
Solid Earth
author_facet J. P. Platt
author_sort J. P. Platt
title Comment on “Channel flow, tectonic overpressure, and exhumation of high-pressure rocks in the Greater Himalayas” by Marques et al. (2018)
title_short Comment on “Channel flow, tectonic overpressure, and exhumation of high-pressure rocks in the Greater Himalayas” by Marques et al. (2018)
title_full Comment on “Channel flow, tectonic overpressure, and exhumation of high-pressure rocks in the Greater Himalayas” by Marques et al. (2018)
title_fullStr Comment on “Channel flow, tectonic overpressure, and exhumation of high-pressure rocks in the Greater Himalayas” by Marques et al. (2018)
title_full_unstemmed Comment on “Channel flow, tectonic overpressure, and exhumation of high-pressure rocks in the Greater Himalayas” by Marques et al. (2018)
title_sort comment on “channel flow, tectonic overpressure, and exhumation of high-pressure rocks in the greater himalayas” by marques et al. (2018)
publisher Copernicus Publications
series Solid Earth
issn 1869-9510
1869-9529
publishDate 2019-02-01
description <p>The upward-tapering channel model proposed by Marques et al. (2018) for the Himalayas has a “base” that forms part of the subducting footwall and therefore does not close the channel. This configuration does not produce return flow, and no dynamic overpressure develops in the channel. The geometrical and kinematic configuration they actually use for their calculations differs from this and is both geologically and mechanically improbable. In addition, the fixed upper boundary condition in their models is mechanically unrealistic and inconsistent with geological and geophysical constraints from the Himalayan orogen. In reality, the dynamic pressures calculated from their model, which exceed lithostatic pressure by as much as 1.5&thinsp;GPa, would cause elastic flexure or permanent deformation of the upper plate. I estimate that a flexural upwarp of 50&thinsp;km of the upper plate would be required to balance forces, which would lead to geologically unrealistic topographic and gravity anomalies. The magnitude of the dynamic overpressure that could be confined is in fact limited by the shear strength of the upper plate in the Himalayas, which is likely to be &lt;&thinsp;120&thinsp;MPa.</p>
url https://www.solid-earth.net/10/357/2019/se-10-357-2019.pdf
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