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Fluid flow with fluid pressure 

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bodyp(t, {\bf r})
and  are not changing in time:

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p(t, {\bf r}) = p({\bf r})

This immediately leads to the stationary fluid velocity 

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body{\bf u}(t, {\bf r})

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: 

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anchoru
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p{\bf u}(t, {\bf r}) = p{\bf u}({\bf r})


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titleDerivation


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The fluid velocity is:

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{\bf u}(t, {\bf r})
=
= M({\bf r}, p, \nabla p) \nabla p

and

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\frac{\partial {\bf u}(t, {\bf r})}{\partial t}= 0

which leads to

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anchoru
.




The fluid temperature 

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bodyT(t, {\bf r})
 is supposed to vary slowly enough to provide quasistatic equilibrium.

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This flow regime is often observed in pipeline fluid flow and reservoir fluid flows


See also

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Physics / Fluid Dynamics 

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