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c(T,p) = \frac{1}{\rho} \left( \frac{\partial \rho}{\partial p} \right)_T = - \frac{1}{V_m} \left( \frac{\partial V_m}{\partial p} \right)_T


There is no universal full-range analytical model for Fluid Compressibility but there is a good number of approximations which can be effectively used in engineering practice.

Approximations

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Incompressible fluidCompressible fluid
Full-Range Proxy Model

Slightly compressible fluidStrongly Compressible Fluid

Real GasIdeal Gas
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c(T, p) = 0
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c(T, p) = c_0 = \rm const


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c(T, p) = \frac{1
}{p} LaTeX Math Block
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c(T, p) = \frac{c_0(T,p)
}{
1+c_0(T,p) \cdot LaTeX Math Block
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p}
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\rho(T, p) = \rho_0(T)
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\rho(T, p) = \rho_0 \cdot \exp \left[ c_0(T) \cdot (p-p_0) \right]



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\rho(T, p) = \frac{\rho_0(T)}{p_0} \cdot p
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\rho(T, p) = \rho_0(T) \cdot \frac{1+c_0(T,p) \, p}{1+c_0(T,p) \, p_0}
Z(T, p) = \frac{p}{p_0}
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Z(T, p) =\frac{p}{p_0}\cdot \exp \left[ - c_0(T) \cdot (p-p_0) \right]


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Z(T, p) = 1
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Z(T, p) = \frac{p}{p_0} \cdot \frac{1+c_0(T, p) \, p_0}{1 + c_0(T,p) \, p}

where

LaTeX Math Inline
bodyc

fluid compressibility

LaTeX Math Inline
body\rho

fluid density

LaTeX Math Inline
bodyZ

Z-factor



Mathematical A number of full-range mathematical models of 
Fluid Compressibility are reviewed  can be found in Fluid Compressibility @model.


The 
multi-phase fluid compressibility is a linear sum of compressibilities of its phases (see multi-phase fluid compressibility @ model).


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Fluid Compressibility of popular petroleum fluids at SPE Standard Conditions (STP):

FluidTypical Range, GPa-1
Natural Gas10,000 
Gas Condensate 100
Oil1 – 10
Water0.44 – 0.51 GPa-1


See also

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Physics / Mechanics / Continuum mechanics / Fluid Mechanics / Fluid Statics

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[ Incompressible fluid ] [ Slightly Compressible Fluid ] [ Strongly Compressible Fluid ] [ Ideal Gas ]

[ Water compressibility (cw) ] [Oil compressibility (co)] [Gas compressibility (cg)]