Speed of sound: Difference between revisions
Jump to navigation
Jump to search
Carl McBride (talk | contribs) mNo edit summary |
Carl McBride (talk | contribs) m (Added subscript) |
||
Line 3: | Line 3: | ||
:<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> |
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