In case the phases have the same pressure the compressibility of multi-phase fluid can be expressed via compressibilities of single-phase fluids as: Compressibility of multiphase fluid in thermodynamic equilibrium at a given pressure
and temperature is a linear sum of its single-phase components: LaTeX Math Block |
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c_f(p, T) = c\sum_w {\,alpha} s_w\alpha +\cdot c_o \, s_o + c_g \, s_g\alpha(p,T) |
where
| -phase volume share, subjected to LaTeX Math Inline |
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body | \sum_{\alpha} s_\alpha = 1 |
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The total multiphase volume: _f V_w, s_w + o \, s_o + V_g \, s_g | where
where are volumes, occupied by individual phases.
The volume fraction of individual phase is defined as: w = \frac{V_w}{V_f}, \ s_o o}{V_f}, \ s_g = \frac{V_g_f This leads to:
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| c_f = \frac{1}{V | _f_f}{\partial p} =
\frac{1}{V | _ffrac{V_w}{p} + 1}{f} \frac{V_op} + \frac{1}{V_f} \frac{V_g}{p} | LaTeX Math Block |
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| c_ffrac{V_w}{V_f}{1}w \frac_w{p}+ \frac{V_o}{V_f}o\alpha} \frac{\partial V_ | o+frac{V_g}{V_f} \frac{1}{V_g} \frac{V_g}{p}sum_\alpha s_\alpha \, c_\alpha |
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In most popular practical case of a 3-phase fluid model this will be:
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c_f = \frac{Vs_w }{V_f} \ frac{1}{V_w} \frac{V_w}{p}, c_w + \frac{Vs_o }{V_f} \ frac{1}{V_o} \frac{V_o}{p}, c_o + \frac{Vs_g }{V_f} \ frac{1}{V_g} \frac{V_g}{p}which leads to LaTeX Math Block Reference |
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| anchor | cf, c_g
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where
mean water phase, oil phase and gas phase.
See also
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Physics / Mechanics / Continuum mechanics / Fluid Mechanics / Fluid Statics / Fluid Compressibility / Fluid Compressibility @model