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- 2019-06-20T14:59:58+02:00 (5 years ago)
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NEMO/trunk/doc/latex/NEMO/subfiles/chap_conservation.tex
r11123 r11151 65 65 % \label{eq:vor_vorticity} 66 66 \int_D {{\textbf {k}}\cdot \frac{1}{e_3 }\nabla \times \left( {\varsigma 67 \;{\ rm {\bf k}}\times {\textbf {U}}_h } \right)\;dv} =067 \;{\mathrm {\mathbf k}}\times {\textbf {U}}_h } \right)\;dv} =0 68 68 \] 69 69 … … 189 189 \[ 190 190 % \label{eq:dynldf_dyn} 191 \int\limits_D {\frac{1}{e_3 }{\ rm {\bf k}}\cdot \nabla \times \left[ {\nabla191 \int\limits_D {\frac{1}{e_3 }{\mathrm {\mathbf k}}\cdot \nabla \times \left[ {\nabla 192 192 _h \left( {A^{lm}\;\chi } \right)-\nabla _h \times \left( {A^{lm}\;\zeta 193 \;{\ rm {\bf k}}} \right)} \right]\;dv} =0193 \;{\mathrm {\mathbf k}}} \right)} \right]\;dv} =0 194 194 \] 195 195 … … 197 197 % \label{eq:dynldf_div} 198 198 \int\limits_D {\nabla _h \cdot \left[ {\nabla _h \left( {A^{lm}\;\chi } 199 \right)-\nabla _h \times \left( {A^{lm}\;\zeta \;{\ rm {\bf k}}} \right)}199 \right)-\nabla _h \times \left( {A^{lm}\;\zeta \;{\mathrm {\mathbf k}}} \right)} 200 200 \right]\;dv} =0 201 201 \] … … 203 203 \[ 204 204 % \label{eq:dynldf_curl} 205 \int_D {{\ rm {\bf U}}_h \cdot \left[ {\nabla _h \left( {A^{lm}\;\chi }206 \right)-\nabla _h \times \left( {A^{lm}\;\zeta \;{\ rm {\bf k}}} \right)}205 \int_D {{\mathrm {\mathbf U}}_h \cdot \left[ {\nabla _h \left( {A^{lm}\;\chi } 206 \right)-\nabla _h \times \left( {A^{lm}\;\zeta \;{\mathrm {\mathbf k}}} \right)} 207 207 \right]\;dv} \leqslant 0 208 208 \] … … 210 210 \[ 211 211 % \label{eq:dynldf_curl2} 212 \mbox{if}\quad A^{lm}=cste\quad \quad \int_D {\zeta \;{\ rm {\bf k}}\cdot212 \mbox{if}\quad A^{lm}=cste\quad \quad \int_D {\zeta \;{\mathrm {\mathbf k}}\cdot 213 213 \nabla \times \left[ {\nabla _h \left( {A^{lm}\;\chi } \right)-\nabla _h 214 \times \left( {A^{lm}\;\zeta \;{\ rm {\bf k}}} \right)} \right]\;dv}214 \times \left( {A^{lm}\;\zeta \;{\mathrm {\mathbf k}}} \right)} \right]\;dv} 215 215 \leqslant 0 216 216 \] … … 220 220 \mbox{if}\quad A^{lm}=cste\quad \quad \int_D {\chi \;\nabla _h \cdot \left[ 221 221 {\nabla _h \left( {A^{lm}\;\chi } \right)-\nabla _h \times \left( 222 {A^{lm}\;\zeta \;{\ rm {\bf k}}} \right)} \right]\;dv} \leqslant 0222 {A^{lm}\;\zeta \;{\mathrm {\mathbf k}}} \right)} \right]\;dv} \leqslant 0 223 223 \] 224 224 … … 260 260 % \label{eq:dynzdf_vor} 261 261 \begin{aligned} 262 & \int_D {\frac{1}{e_3 }{\ rm {\bf k}}\cdot \nabla \times \left( {\frac{1}{e_3263 }\frac{\partial }{\partial k}\left( {\frac{A^{vm}}{e_3 }\frac{\partial {\ rm264 {\ bf U}}_h }{\partial k}} \right)} \right)\;dv} =0 \\265 & \int_D {\zeta \,{\ rm {\bf k}}\cdot \nabla \times \left( {\frac{1}{e_3266 }\frac{\partial }{\partial k}\left( {\frac{A^{vm}}{e_3 }\frac{\partial {\ rm267 {\ bf U}}_h }{\partial k}} \right)} \right)\;dv} \leq 0 \\262 & \int_D {\frac{1}{e_3 }{\mathrm {\mathbf k}}\cdot \nabla \times \left( {\frac{1}{e_3 263 }\frac{\partial }{\partial k}\left( {\frac{A^{vm}}{e_3 }\frac{\partial {\mathrm 264 {\mathbf U}}_h }{\partial k}} \right)} \right)\;dv} =0 \\ 265 & \int_D {\zeta \,{\mathrm {\mathbf k}}\cdot \nabla \times \left( {\frac{1}{e_3 266 }\frac{\partial }{\partial k}\left( {\frac{A^{vm}}{e_3 }\frac{\partial {\mathrm 267 {\mathbf U}}_h }{\partial k}} \right)} \right)\;dv} \leq 0 \\ 268 268 \end{aligned} 269 269 \] … … 273 273 \begin{aligned} 274 274 &\int_D {\nabla \cdot \left( {\frac{1}{e_3 }\frac{\partial }{\partial 275 k}\left( {\frac{A^{vm}}{e_3 }\frac{\partial {\ rm {\bf U}}_h }{\partial k}}275 k}\left( {\frac{A^{vm}}{e_3 }\frac{\partial {\mathrm {\mathbf U}}_h }{\partial k}} 276 276 \right)} \right)\;dv} =0 \\ 277 277 & \int_D {\chi \;\nabla \cdot \left( {\frac{1}{e_3 }\frac{\partial }{\partial 278 k}\left( {\frac{A^{vm}}{e_3 }\frac{\partial {\ rm {\bf U}}_h }{\partial k}}278 k}\left( {\frac{A^{vm}}{e_3 }\frac{\partial {\mathrm {\mathbf U}}_h }{\partial k}} 279 279 \right)} \right)\;dv} \leq 0 \\ 280 280 \end{aligned}
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