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Fluid flow with fluid pressure
and are not changing in time: LaTeX Math Block |
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p(t, {\bf r}) = p({\bf r}) |
This immediately leads to the stationary fluid velocity
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:
LaTeX Math Block |
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p{\bf u}(t, {\bf r}) = p{\bf u}({\bf r}) |
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borderColor | wheat |
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borderWidth | 10 |
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| The fluid velocity is: LaTeX Math Block |
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| {\bf u}(t, {\bf r}) |
| == M({\bf r}, p, \nabla p) \nabla p |
and LaTeX Math Block |
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| \frac{\partial {\bf u}(t, {\bf r})}{\partial t}= 0 |
which leads to LaTeX Math Block Reference |
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| . |
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The fluid temperature
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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