DJL equations: Difference between revisions
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== Boussinesq with constant background velocity <math>U_0</math> == | == Boussinesq with constant background velocity <math>U_0</math> == | ||
<math>\nabla^2 \eta + \frac{N^2(z-\eta)}{U_0^2} = 0</math> | <math>\nabla^2 \eta + \frac{N^2(z-\eta)}{U_0^2} = 0</math> | ||
where <math> N^2(z) = -\frac{g}{/rho_0}\frac{d\rho}{dz}</math> | |||
== Boussinesq with non-constant background current <math>U_(z)</math> == | |||
Revision as of 11:26, 7 July 2011
Boussinesq with constant background velocity
where
