Convergent flow in a two-layer system and plateau development

In order to describe the development of plateaus such as the Tibet and the Altiplano we extend the two-layer model used in a previous paper [C. A. Perazzo and J. Gratton, Phys. Fluids22, 056603 (2010)] to reproduce the evolution of mountain ranges. As before, we consider the convergent motion of a s...

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Autores principales: Gratton, J., Perazzo, C.A.
Formato: Artículo publishedVersion
Lenguaje:Inglés
Publicado: 2011
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Acceso en línea:http://hdl.handle.net/20.500.12110/paper_10706631_v23_n4_p_Gratton
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spelling paperaa:paper_10706631_v23_n4_p_Gratton2023-06-12T16:49:26Z Convergent flow in a two-layer system and plateau development Phys. Fluids 2011;23(4) Gratton, J. Perazzo, C.A. Approximate formulas Liquid layer Lithospheric Mountain ranges Nonlinear differential equation Traveling wave Two layer model Two-layer systems Upper mantle Approximation algorithms Differential equations Liquids Viscosity Nonlinear equations In order to describe the development of plateaus such as the Tibet and the Altiplano we extend the two-layer model used in a previous paper [C. A. Perazzo and J. Gratton, Phys. Fluids22, 056603 (2010)] to reproduce the evolution of mountain ranges. As before, we consider the convergent motion of a system of two liquid layers to simulate the crust and the upper mantle that form a lithospheric plate, but now we assume that the viscosity of the crust falls off abruptly at a specified depth. We derive a nonlinear differential equation for the evolution of the thickness of the crust. The solution of this equation shows that the process consists of a first stage in which a peaked range is formed and grows until its root reaches the depth where its viscosity drops. After that the range ceases to grow in height and a flat plateau appears at its top. In this second stage the plateau width increases linearly with time as its sides move outward as traveling waves. We derive simple approximate formulas for various properties of the plateau and its evolution. © 2011 American Institute of Physics. Fil:Gratton, J. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. Fil:Perazzo, C.A. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. 2011 info:eu-repo/semantics/article info:ar-repo/semantics/artículo info:eu-repo/semantics/publishedVersion application/pdf eng info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_10706631_v23_n4_p_Gratton
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
language Inglés
orig_language_str_mv eng
topic Approximate formulas
Liquid layer
Lithospheric
Mountain ranges
Nonlinear differential equation
Traveling wave
Two layer model
Two-layer systems
Upper mantle
Approximation algorithms
Differential equations
Liquids
Viscosity
Nonlinear equations
spellingShingle Approximate formulas
Liquid layer
Lithospheric
Mountain ranges
Nonlinear differential equation
Traveling wave
Two layer model
Two-layer systems
Upper mantle
Approximation algorithms
Differential equations
Liquids
Viscosity
Nonlinear equations
Gratton, J.
Perazzo, C.A.
Convergent flow in a two-layer system and plateau development
topic_facet Approximate formulas
Liquid layer
Lithospheric
Mountain ranges
Nonlinear differential equation
Traveling wave
Two layer model
Two-layer systems
Upper mantle
Approximation algorithms
Differential equations
Liquids
Viscosity
Nonlinear equations
description In order to describe the development of plateaus such as the Tibet and the Altiplano we extend the two-layer model used in a previous paper [C. A. Perazzo and J. Gratton, Phys. Fluids22, 056603 (2010)] to reproduce the evolution of mountain ranges. As before, we consider the convergent motion of a system of two liquid layers to simulate the crust and the upper mantle that form a lithospheric plate, but now we assume that the viscosity of the crust falls off abruptly at a specified depth. We derive a nonlinear differential equation for the evolution of the thickness of the crust. The solution of this equation shows that the process consists of a first stage in which a peaked range is formed and grows until its root reaches the depth where its viscosity drops. After that the range ceases to grow in height and a flat plateau appears at its top. In this second stage the plateau width increases linearly with time as its sides move outward as traveling waves. We derive simple approximate formulas for various properties of the plateau and its evolution. © 2011 American Institute of Physics.
format Artículo
Artículo
publishedVersion
author Gratton, J.
Perazzo, C.A.
author_facet Gratton, J.
Perazzo, C.A.
author_sort Gratton, J.
title Convergent flow in a two-layer system and plateau development
title_short Convergent flow in a two-layer system and plateau development
title_full Convergent flow in a two-layer system and plateau development
title_fullStr Convergent flow in a two-layer system and plateau development
title_full_unstemmed Convergent flow in a two-layer system and plateau development
title_sort convergent flow in a two-layer system and plateau development
publishDate 2011
url http://hdl.handle.net/20.500.12110/paper_10706631_v23_n4_p_Gratton
work_keys_str_mv AT grattonj convergentflowinatwolayersystemandplateaudevelopment
AT perazzoca convergentflowinatwolayersystemandplateaudevelopment
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