CMS-Flow:Wave Eqs: Difference between revisions

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Taking into account the effect of an ambient horizontal current or wave behavior, CMS-Wave is based on the steady wave-action balance equation (Mase 2001)
Taking into account the effect of an ambient horizontal current or wave behavior, CMS-Wave is based on the steady wave-action balance equation (Mase 2001)


         <math> \frac{\partial c_x N  }{\partial x}
         <math> \frac{\partial (c_x N) }{\partial x}
+  \frac{\partial c_y N  }{\partial y}
+  \frac{\partial (c_y N) }{\partial y}
+  \frac{\partial c_{\theta} N  }{\partial \theta}  
+  \frac{\partial (c_{\theta} N) }{\partial \theta}  
= \frac{\kappa}{2 \sigma}  \biggl[ (c c_g \cos ^2 \theta N_y)_y - \frac{c c_g}{2} \cos ^2 \theta N_{yy} \biggr]
= \frac{\kappa}{2 \sigma}  \biggl[ (c c_g \cos ^2 \theta N_y)_y - \frac{c c_g}{2} \cos ^2 \theta N_{yy} \biggr]
- \epsilon_b N - S </math>
- \epsilon_b N - S </math>

Revision as of 22:19, 17 May 2010

Wave-action balance equation with diffraction

Taking into account the effect of an ambient horizontal current or wave behavior, CMS-Wave is based on the steady wave-action balance equation (Mase 2001)

        (cxN)x+(cyN)y+(cθN)θ=κ2σ[(ccgcos2θNy)yccg2cos2θNyy]ϵbNS

for j=1,2

        (hUi)t+(hUiUj)xjϵij3fcUjh=ghηxjhρ0paxj+xj(νthUixj)+τiρ  

for i=1,2 and j=1,2

Symbol Description
σ Wave frequency
N Wave action
E Spectral wave density
c Wave celerity
cg Wave group velocity

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