Changeset 10406 for NEMO/trunk/doc/latex/NEMO/subfiles/chap_DIU.tex
- Timestamp:
- 2018-12-18T11:25:09+01:00 (5 years ago)
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- NEMO/trunk/doc/latex
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- 4 edited
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NEMO/trunk/doc/latex
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NEMO/trunk/doc/latex/NEMO/subfiles
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NEMO/trunk/doc/latex/NEMO/subfiles/chap_DIU.tex
r10354 r10406 61 61 The warm layer is calculated using the model of \citet{Takaya_al_JGR10} (TAKAYA10 model hereafter). 62 62 This is a simple flux based model that is defined by the equations 63 \begin{ eqnarray}63 \begin{align} 64 64 \frac{\partial{\Delta T_{\rm{wl}}}}{\partial{t}}&=&\frac{Q(\nu+1)}{D_T\rho_w c_p 65 65 \nu}-\frac{(\nu+1)ku^*_{w}f(L_a)\Delta T}{D_T\Phi\!\left(\frac{D_T}{L}\right)} \mbox{,} 66 66 \label{eq:ecmwf1} \\ 67 67 L&=&\frac{\rho_w c_p u^{*^3}_{w}}{\kappa g \alpha_w Q }\mbox{,}\label{eq:ecmwf2} 68 \end{ eqnarray}68 \end{align} 69 69 where $\Delta T_{\rm{wl}}$ is the temperature difference between the top of the warm layer and the depth $D_T=3$\,m at which there is assumed to be no diurnal signal. 70 70 In equation (\autoref{eq:ecmwf1}) $\alpha_w=2\times10^{-4}$ is the thermal expansion coefficient of water,
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