A general solution of the equations of hydrodynamics

Author:

Milne-Thomson L. M.

Abstract

Consider a fluid of constant viscosity μ. If the fluid is incompressible, we suppose it to move in a conservative field in which the force per unit mass is - ∇Ω. If the fluid is compressible, we suppose the field of force to be absent. Both cases are included if we write V = ερΩ, where ε = 1 for an incompressible fluid, and ε = 0 for a compressible fluid. The equation of continuity

Publisher

Cambridge University Press (CUP)

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics

Reference2 articles.

1. Milne-Thomson, L. M. 1942 Consistency equations for the stresses in isotropic elastic and plastic materials.J. London Math. Soc. 17,115–128.

2. Milne-Thomson, L. M. 1955 Theoretical Hydrodynamics ,3rd Ed. London:Macmillan.

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