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The condition of mechanical equilibrium for a non-spherical interface between phases with a non-diagonal stress tensor. / Rusanov, Anatoly I.; Shchekin, Alexander K.

In: Colloids and Surfaces A: Physicochemical and Engineering Aspects, Vol. 192, No. 1-3, 30.11.2001, p. 357-362.

Research output: Contribution to journal › Short survey › peer-review

Harvard

Rusanov, AI & Shchekin, AK 2001, 'The condition of mechanical equilibrium for a non-spherical interface between phases with a non-diagonal stress tensor', Colloids and Surfaces A: Physicochemical and Engineering Aspects, vol. 192, no. 1-3, pp. 357-362. https://doi.org/10.1016/S0927-7757(01)00736-1

APA

Rusanov, A. I., & Shchekin, A. K. (2001). The condition of mechanical equilibrium for a non-spherical interface between phases with a non-diagonal stress tensor. Colloids and Surfaces A: Physicochemical and Engineering Aspects, 192(1-3), 357-362. https://doi.org/10.1016/S0927-7757(01)00736-1

Vancouver

Rusanov AI, Shchekin AK. The condition of mechanical equilibrium for a non-spherical interface between phases with a non-diagonal stress tensor. Colloids and Surfaces A: Physicochemical and Engineering Aspects. 2001 Nov 30;192(1-3):357-362. https://doi.org/10.1016/S0927-7757(01)00736-1

Author

Rusanov, Anatoly I. ; Shchekin, Alexander K. / The condition of mechanical equilibrium for a non-spherical interface between phases with a non-diagonal stress tensor. In: Colloids and Surfaces A: Physicochemical and Engineering Aspects. 2001 ; Vol. 192, No. 1-3. pp. 357-362.

BibTeX

@article{4300fec5ecab4b31bc3b288abc54c60f,
title = "The condition of mechanical equilibrium for a non-spherical interface between phases with a non-diagonal stress tensor",
abstract = "A compact form for the condition of mechanical equilibrium for arbitrary curved interfaces has been formulated in the case when the bulk pressures are non-diagonal local tensors. This form of the condition is applicable to a non-spherical interface between fluid or solid phases, without or with arbitrary number of any external fields. The equilibrium condition has been transformed into a set of differential equations for the tangential and transverse components of the mechanical surface tension and bulk pressure tensors at a dividing surface. One condition simplifies to the usual Laplace equation of capillarity for the transverse direction across the interface, while the other conditions relate to the tangential equilibrium state of the fluid. The amendment of the definition of a dividing surface has been given.",
keywords = "Fluids in external fields, Laplace equation, Non-spherical interfaces, Surface tension",
author = "Rusanov, {Anatoly I.} and Shchekin, {Alexander K.}",
year = "2001",
month = nov,
day = "30",
doi = "10.1016/S0927-7757(01)00736-1",
language = "English",
volume = "192",
pages = "357--362",
journal = "Colloids and Surfaces A: Physicochemical and Engineering Aspects",
issn = "0927-7757",
publisher = "Elsevier",
number = "1-3",

}

RIS

TY - JOUR

T1 - The condition of mechanical equilibrium for a non-spherical interface between phases with a non-diagonal stress tensor

AU - Rusanov, Anatoly I.

AU - Shchekin, Alexander K.

PY - 2001/11/30

Y1 - 2001/11/30

N2 - A compact form for the condition of mechanical equilibrium for arbitrary curved interfaces has been formulated in the case when the bulk pressures are non-diagonal local tensors. This form of the condition is applicable to a non-spherical interface between fluid or solid phases, without or with arbitrary number of any external fields. The equilibrium condition has been transformed into a set of differential equations for the tangential and transverse components of the mechanical surface tension and bulk pressure tensors at a dividing surface. One condition simplifies to the usual Laplace equation of capillarity for the transverse direction across the interface, while the other conditions relate to the tangential equilibrium state of the fluid. The amendment of the definition of a dividing surface has been given.

AB - A compact form for the condition of mechanical equilibrium for arbitrary curved interfaces has been formulated in the case when the bulk pressures are non-diagonal local tensors. This form of the condition is applicable to a non-spherical interface between fluid or solid phases, without or with arbitrary number of any external fields. The equilibrium condition has been transformed into a set of differential equations for the tangential and transverse components of the mechanical surface tension and bulk pressure tensors at a dividing surface. One condition simplifies to the usual Laplace equation of capillarity for the transverse direction across the interface, while the other conditions relate to the tangential equilibrium state of the fluid. The amendment of the definition of a dividing surface has been given.

KW - Fluids in external fields

KW - Laplace equation

KW - Non-spherical interfaces

KW - Surface tension

UR - http://www.scopus.com/inward/record.url?scp=0035976424&partnerID=8YFLogxK

U2 - 10.1016/S0927-7757(01)00736-1

DO - 10.1016/S0927-7757(01)00736-1

M3 - Short survey

AN - SCOPUS:0035976424

VL - 192

SP - 357

EP - 362

JO - Colloids and Surfaces A: Physicochemical and Engineering Aspects

JF - Colloids and Surfaces A: Physicochemical and Engineering Aspects

SN - 0927-7757

IS - 1-3

ER -

ID: 26002045