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@wikipedia


A measure of relative change in density 

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body\rho
 or  molar volume  
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bodyV_m
 under a unit 
pressure 
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bodyp
 variation:

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K = \rho \cdot \left( \frac{\partial p}{\partial \rho} \right) = - V_m \cdot \left( \frac{\partial p}{\partial V_m} \right)
SymbolDimensionSI unitsOil metric unitsOil field units

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bodyK
 or 
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bodyB

M1 L-1 T-2PaGPa

psi


Bulk modulus measures resistance of Continuum body to compression/decompression and is inverse to Compressibility 

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bodyc
:


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K = \frac{1}{c}


Bulk modulus depends on the thermodynamic conditions at which it is measured and as such is not a material property.

The two major deformation processes of the medium are isothermal and isentropic which result in different values of Bulk modulus:

Isothermal bulk modulusIsentropic bulk modulus

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bodyT = \rm const

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bodyS = \rm const

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K_T = \rho \cdot \left( \frac{\partial p}{\partial \rho} \right)_T
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K_S = \rho \cdot \left( \frac{\partial p}{\partial \rho} \right)_S


Both 

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bodyK_T
 and 
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bodyK_S
 are not dependent on the amount of chemical substance and defined under specific conditions of thermodynamic process and 
as such are the material properties and properly tabulated for the vast majority of materials.

In engineering practise, when the term Bulk modulus is used as material property it normally means Isothermal Compressibility

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bodyK=K_T
.

For isotropic materials it is related to Young modulus (E) and Poisson's ratio (ν) as:

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anchorKE
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K_T = \frac{E}{3 \, (1- 2\, \nu)}


See also


Physics / Mechanics /  Continuum mechanics / Continuum Body / Deformation

Solid Mechanics ] [ Fluid Mechanics]

[Compressibility] [ Young modulus (E) ]Poisson's ratio (ν) ]

Isothermal Compressibility ][ Isentropic Compressibility ]

[Fluid compressibility] [Pore compressibility] [Total compressibility]