Speed of sound: Difference between revisions

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:<math>c =  \sqrt{ \left. \frac{\partial p}{\partial \rho} \right\vert_S } = \sqrt{ \frac{B_S}{\rho} }</math>
:<math>c =  \sqrt{ \left. \frac{\partial p}{\partial \rho} \right\vert_S } = \sqrt{ \frac{B_S}{\rho} }</math>


where <math>B</math> is the adiabatic [[Compressibility |bulk modulus]], given by
where <math>B_S</math> is the adiabatic [[Compressibility |bulk modulus]], given by


:<math>B_S = \frac{C_p}{C_V} B_T</math>
:<math>B_S = \frac{C_p}{C_V} B_T</math>
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:<math>c =  \sqrt{  \frac{C_p B_T}{C_V \rho} }</math>
:<math>c =  \sqrt{  \frac{C_p B_T}{C_V \rho} }</math>
==See also==
*[[Cole equation of state]]


==References==
==References==

Latest revision as of 15:59, 23 May 2012

The speed of sound () can be written as:

where is the adiabatic bulk modulus, given by

where is the heat capacity and is the isothermal bulk modulus, leading to

See also[edit]

References[edit]