Wave Momentum Flux: Difference between revisions
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<u> Momentum flux in | <u> Momentum flux in potential flow </u> | ||
<center><math> \frac{d\overline{M(t)}}{dt} = \rho \frac{d}{dt} \iiint_V(t) \bar V dV = \rho \iiint_V(t) \frac{\partial\bar{V}}{\partial t} dV + \rho \ | <center><math> \frac{d\overline{M(t)}}{dt} = \rho \frac{d}{dt} \iiint_V(t) \bar V dV = \rho \iiint_V(t) \frac{\partial\bar{V}}{\partial t} dV + \rho \oint_{S(t)} \bar{V} U_n dS, </math></center> | ||
by virtue of the transport theorem | |||
Invoking Euler's equations in inviscid flow | Invoking Euler's equations in inviscid flow |
Revision as of 22:36, 16 February 2007
Momentum flux in potential flow
by virtue of the transport theorem
Invoking Euler's equations in inviscid flow
We may recast the rate of change of the momentum ([math]\displaystyle{ \equiv \, }[/math] momentum flux) in the form