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Changeset 11151 for NEMO/trunk/doc/latex/NEMO/subfiles/chap_conservation.tex – NEMO

Ignore:
Timestamp:
2019-06-20T14:59:58+02:00 (5 years ago)
Author:
nicolasmartin
Message:

New version of NEMO_manual.tex
New class scrreport for the document (KOMA-script version of default report)
Foreword is now placed before ToC.
All figures are configured with 1.0\textwidth as default.
For compatibilty, \frontmatter, \mainmatter and \backmatter cmds have been removed and old fonts in LaTeX subfiles have been replaced

  • \bf -> \mathbf or \bfseries
  • \it -> \itshape
  • \rm -> \mathrm or \rmfamily
  • \tt -> \ttfamily
File:
1 edited

Legend:

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  • NEMO/trunk/doc/latex/NEMO/subfiles/chap_conservation.tex

    r11123 r11151  
    6565  % \label{eq:vor_vorticity} 
    6666  \int_D {{\textbf {k}}\cdot \frac{1}{e_3 }\nabla \times \left( {\varsigma 
    67         \;{\rm {\bf k}}\times {\textbf {U}}_h } \right)\;dv} =0 
     67        \;{\mathrm {\mathbf k}}\times {\textbf {U}}_h } \right)\;dv} =0 
    6868\] 
    6969 
     
    189189\[ 
    190190  % \label{eq:dynldf_dyn} 
    191   \int\limits_D {\frac{1}{e_3 }{\rm {\bf k}}\cdot \nabla \times \left[ {\nabla 
     191  \int\limits_D {\frac{1}{e_3 }{\mathrm {\mathbf k}}\cdot \nabla \times \left[ {\nabla 
    192192        _h \left( {A^{lm}\;\chi } \right)-\nabla _h \times \left( {A^{lm}\;\zeta 
    193             \;{\rm {\bf k}}} \right)} \right]\;dv} =0 
     193            \;{\mathrm {\mathbf k}}} \right)} \right]\;dv} =0 
    194194\] 
    195195 
     
    197197  % \label{eq:dynldf_div} 
    198198  \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)} 
    200200    \right]\;dv} =0 
    201201\] 
     
    203203\[ 
    204204  % \label{eq:dynldf_curl} 
    205   \int_D {{\rm {\bf U}}_h \cdot \left[ {\nabla _h \left( {A^{lm}\;\chi } 
    206         \right)-\nabla _h \times \left( {A^{lm}\;\zeta \;{\rm {\bf k}}} \right)} 
     205  \int_D {{\mathrm {\mathbf U}}_h \cdot \left[ {\nabla _h \left( {A^{lm}\;\chi } 
     206        \right)-\nabla _h \times \left( {A^{lm}\;\zeta \;{\mathrm {\mathbf k}}} \right)} 
    207207    \right]\;dv} \leqslant 0 
    208208\] 
     
    210210\[ 
    211211  % \label{eq:dynldf_curl2} 
    212   \mbox{if}\quad A^{lm}=cste\quad \quad \int_D {\zeta \;{\rm {\bf k}}\cdot 
     212  \mbox{if}\quad A^{lm}=cste\quad \quad \int_D {\zeta \;{\mathrm {\mathbf k}}\cdot 
    213213    \nabla \times \left[ {\nabla _h \left( {A^{lm}\;\chi } \right)-\nabla _h 
    214         \times \left( {A^{lm}\;\zeta \;{\rm {\bf k}}} \right)} \right]\;dv} 
     214        \times \left( {A^{lm}\;\zeta \;{\mathrm {\mathbf k}}} \right)} \right]\;dv} 
    215215  \leqslant 0 
    216216\] 
     
    220220  \mbox{if}\quad A^{lm}=cste\quad \quad \int_D {\chi \;\nabla _h \cdot \left[ 
    221221      {\nabla _h \left( {A^{lm}\;\chi } \right)-\nabla _h \times \left( 
    222           {A^{lm}\;\zeta \;{\rm {\bf k}}} \right)} \right]\;dv} \leqslant 0 
     222          {A^{lm}\;\zeta \;{\mathrm {\mathbf k}}} \right)} \right]\;dv} \leqslant 0 
    223223\] 
    224224 
     
    260260  % \label{eq:dynzdf_vor} 
    261261  \begin{aligned} 
    262     & \int_D {\frac{1}{e_3 }{\rm {\bf k}}\cdot \nabla \times \left( {\frac{1}{e_3 
    263           }\frac{\partial }{\partial k}\left( {\frac{A^{vm}}{e_3 }\frac{\partial {\rm 
    264                   {\bf U}}_h }{\partial k}} \right)} \right)\;dv} =0 \\ 
    265     & \int_D {\zeta \,{\rm {\bf k}}\cdot \nabla \times \left( {\frac{1}{e_3 
    266           }\frac{\partial }{\partial k}\left( {\frac{A^{vm}}{e_3 }\frac{\partial {\rm 
    267                   {\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 \\ 
    268268  \end{aligned} 
    269269\] 
     
    273273  \begin{aligned} 
    274274    &\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}} 
    276276          \right)} \right)\;dv} =0 \\ 
    277277    & \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}} 
    279279          \right)} \right)\;dv} \leq 0 \\ 
    280280  \end{aligned} 
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