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@wikipedia


Stationary Fluid flow when  with fluid pressure and temperature across reservoir do not change  pressure 

LaTeX Math Inline
bodyp(t, {\bf r})
 is not changing in time:

T
LaTeX Math Block
anchorp
alignmentleft
p(t, {\bf r}) = p({\rmbf const
LaTeX Math Block
alignmentleft
r})

This immediately leads to stationary fluid velocity 

LaTeX Math Inline
body{\bf u}(t,

...

{\bf

...

r})

...

...

LaTeX Math Block
anchoru
alignmentleft
{\rhobf u}(t, {\bf r}) = \rm const

Well production or injection resulting in steady state flow is characterised by:

{\bf u}({\bf r})



Expand
titleDerivation


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In the most general case (both reservoir and pipelines) the fluid velocity is a function of pressure and pressure gradient and can be written as:

LaTeX Math Block
anchor1

...

alignmentleft

...

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

...

constant flow rate

F({\bf r}, p, \nabla p)

with right side not dependent on time in stationary flow:

LaTeX Math Block
anchor1

...

alignmentleft

...

\frac{\partial {\bf u}(t

...

, 

...

LaTeX Math Block
alignmentleft
p_{wf}(t) = p_{wf} = \rm const

...

{\bf r})}{\partial t}= 0

which leads to

LaTeX Math Block Reference
anchoru
.



The fluid temperature 

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


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

See also

...

Physics / Fluid Dynamics 

Steady State Well Flow Regime (SS) ]