Speed of sound: Difference between revisions
		
		
		
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| Carl McBride (talk | contribs) mNo edit summary | Carl McBride (talk | contribs)  m (Added subscript) | ||
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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> | 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> | ||
| Line 11: | Line 11: | ||
| :<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== | ==See also== | ||
| *[Cole equation of state]] | *[[Cole equation of state]] | ||
| ==References== | ==References== | ||
Latest revision as of 14:59, 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