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Published online by Cambridge University Press: 24 October 2008
The Navier–Stokes equations governing the motion of viscous compressible fluids are
where ρ is the density, q is the velocity vector, V is the scalar potential of the external force field, I is the idemfactor and Φ is the stress-tensor
Milne-Thomson ((l)) has given a general solution of (1) and (2) in the form