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K = \frac{1}{c}

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

The most popular material compressibilities are:

Isothermal CompressibilityIsentropic Compressibility

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bodyT = \rm const

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bodyS = \rm const


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c_T = \frac{1}{\rho} \left( \frac{\partial \rho}{\partial p} \right)_T



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c_S = \frac{1}{\rho} \left( \frac{\partial \rho}{\partial p} \right)_S


See also

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Physics / Mechanics / Continuum mechanics / Continuum body