On the Navier-Stokes equations for water

In general, the existence of entropy imposes restrictions on the constitutive functions in the Navier-Stokes equations. In this paper, it is shown that if the energy per unit mass is a function of the temperature T only, then the pressure p is an arbitrary function of the density ρ multiplied by the...

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Main Author: S. Piekarski
Format: Article
Language:English
Published: Institute of Fundamental Technological Research Polish Academy of Sciences 2014-03-01
Series:Archives of Acoustics
Subjects:
Online Access:https://acoustics.ippt.pan.pl/index.php/aa/article/view/672
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author S. Piekarski
author_facet S. Piekarski
author_sort S. Piekarski
collection DOAJ
description In general, the existence of entropy imposes restrictions on the constitutive functions in the Navier-Stokes equations. In this paper, it is shown that if the energy per unit mass is a function of the temperature T only, then the pressure p is an arbitrary function of the density ρ multiplied by the temperature T. However, for many fluids with the properties radically different than ideal gases (the best example here is water) the pressure as a function of ρ and T is not of the form p0(ρ)T. Therefore the energy density per unit mass in the Navier-Stokes equations for water should depend also on the mass density and the explicit form of this dependence requires further discussion.
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spelling doaj-art-92e928149bfb4986b6ec8e8717da0bf62025-08-20T02:39:19ZengInstitute of Fundamental Technological Research Polish Academy of SciencesArchives of Acoustics0137-50752300-262X2014-03-01312On the Navier-Stokes equations for waterS. Piekarski0Institute of Fundamental Technological Research Polish Academy of SciencesIn general, the existence of entropy imposes restrictions on the constitutive functions in the Navier-Stokes equations. In this paper, it is shown that if the energy per unit mass is a function of the temperature T only, then the pressure p is an arbitrary function of the density ρ multiplied by the temperature T. However, for many fluids with the properties radically different than ideal gases (the best example here is water) the pressure as a function of ρ and T is not of the form p0(ρ)T. Therefore the energy density per unit mass in the Navier-Stokes equations for water should depend also on the mass density and the explicit form of this dependence requires further discussion.https://acoustics.ippt.pan.pl/index.php/aa/article/view/672Gibbs identitythermodynamicsconstitutive functions for water
spellingShingle S. Piekarski
On the Navier-Stokes equations for water
Archives of Acoustics
Gibbs identity
thermodynamics
constitutive functions for water
title On the Navier-Stokes equations for water
title_full On the Navier-Stokes equations for water
title_fullStr On the Navier-Stokes equations for water
title_full_unstemmed On the Navier-Stokes equations for water
title_short On the Navier-Stokes equations for water
title_sort on the navier stokes equations for water
topic Gibbs identity
thermodynamics
constitutive functions for water
url https://acoustics.ippt.pan.pl/index.php/aa/article/view/672
work_keys_str_mv AT spiekarski onthenavierstokesequationsforwater