\batchmode

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\RequirePackage{ifthen}


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\Dtitle[SPMODEL µåÌÌÀõ¿å¥â¥Ç¥ë¤Î¥Æ¥¹¥È]
{SPMODEL ¤Î°ì´Ä¤È¤·¤Æ¤ÎµåÌÌÀõ¿å¥â¥Ç¥ë¤òÍÑ¤¤¤¿ Williamson et al. (1992) ¤Î¥Æ¥¹¥È}
\Dauthor[¾®¹â Àµ»Ì]{¾®¹â Àµ»Ì}            % Ãø¼Ô
\Ddate{2005 Ç¯ 5 ·î 11 Æü ºîÀ®³«»Ï}       % ÆüÉÕ
\Dnoparindent                             % ÃÊÍî¤Î»ú²¼¤²¤ò¤·¤Ê¤¤




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{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1727}%
$\displaystyle \frac{\mbox{max}_{all \lambda, \phi}|(h(\lambda, \phi) - h_{T}(\lambda, \phi)|}
{\mbox{max}_{all \lambda, \phi}
|h_{T}(\lambda, \Phi)|}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1729}%
$\displaystyle l_{1}(\Dvect{v})$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1731}%
$\displaystyle \frac{I[
\sqrt{(u(\lambda, \phi) - u_{T}(\lambda, \Phi))^{2}+
(v(\lambda, \phi) - v_{T}(\lambda, \Phi))^{2}}]}
{I[\sqrt{u_{T}(\lambda, \Phi)^{2} + v_{T}(\lambda, \Phi)^{2}}]},$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1732}%
$\displaystyle l_{2}(\Dvect{v})$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1734}%
$\displaystyle \frac{\sqrt{I[
(u(\lambda, \phi) - u_{T}(\lambda, \Phi))^{2}+
(v(\lambda, \phi) - v_{T}(\lambda, \Phi))^{2}]}}
{\sqrt{I[u_{T}(\lambda, \Phi)^{2} + v_{T}(\lambda, \Phi)^{2}]}},$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1735}%
$\displaystyle l_{\infty}(\Dvect{v})$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1737}%
$\displaystyle \frac{\mbox{max}_{all \lambda, \phi}
[(u(\lambda, \phi) - u_{T}(\lambda, \Phi))^{2}+
(v(\lambda, \phi) - v_{T}(\lambda, \Phi))^{2}]}
{\mbox{max}_{all \lambda, \phi}
[u_{T}(\lambda, \Phi)^{2} + v_{T}(\lambda, \Phi)^{2}]}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline883}%
$h_{T}(\lambda, \Phi)$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline885}%
$T$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline887}%
$I(h)$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline889}%
$h(\lambda, \phi)$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmldisplayA{displaymath246}%
\begin{displaymath}
  I(h) = \frac{1}{4\pi}\int _{0}^{2\pi}\int _{-\pi/2}^{\pi/2}
          h(\lambda, \phi)\sin \phi \Dd \phi \Dd \lambda
\end{displaymath}%
\lthtmldisplayZ
\lthtmlcheckvsize\clearpage}

\stepcounter{subsection}
{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline891}%
$\cos$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline893}%
$u, v$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1749}%
$\displaystyle u$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1751}%
$\displaystyle u_{0}(\cos \phi \cos \alpha + \sin \phi \cos \lambda \sin \alpha),$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1752}%
$\displaystyle v$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1754}%
$\displaystyle - u_{0}\sin \lambda \sin \alpha$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1756}%
$\displaystyle \psi$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1758}%
$\displaystyle - a u_{0}
(\sin \phi \cos \alpha - \cos \lambda \cos \phi \sin \alpha),$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1759}%
$\displaystyle \chi$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1761}%
$\displaystyle 0$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline899}%
$\alpha $%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmldisplayA{displaymath262}%
\begin{displaymath}
  h = \left\{
\begin{array}{ll}
  (h_{0}/2)( 1 + \cos (\pi r/R) ) & (r < R) \\
  0                               & (r \ge R)
\end{array}
\right.
\end{displaymath}%
\lthtmldisplayZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmldisplayA{displaymath268}%
\begin{displaymath}
  r = a \arccos (\sin \phi _{c}\sin \phi + 
                 \cos \phi _{c}\cos \phi \cos (\lambda -\lambda _{c}))
\end{displaymath}%
\lthtmldisplayZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline903}%
$0, \quad 0.05, \quad \pi/2 - 0.05,\quad \pi/2$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline905}%
$u_{0}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline907}%
$2\pi a/(12$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline909}%
${}^{-1}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline911}%
$h_{0}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline913}%
$1000$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline915}%
$\lambda _{c}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline917}%
$3\pi/2$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline919}%
$\phi _{c}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline921}%
$0$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline923}%
$R$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline925}%
$a/3$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

\stepcounter{subsection}
{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1833}%
$\displaystyle - u_{0}\sin \lambda \sin \alpha,$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1834}%
$\displaystyle h$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1836}%
$\displaystyle h_{0} - \left(a\Omega u_{0} + \frac{u_{0}^{2}}{2}\right)
(-\cos \lambda \cos \phi \sin \alpha + \sin \phi \cos \alpha)^{2}/g.$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmldisplayA{displaymath312}%
\begin{displaymath}
  f = 2\Omega(-\cos \lambda \cos \phi \sin \alpha + \sin \phi \cos \alpha).
\end{displaymath}%
\lthtmldisplayZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline943}%
$2.94\times 10^{4}/g$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

\stepcounter{subsection}
{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline945}%
$(\lambda ', \phi')$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline947}%
$u', v', h'$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline951}%
$(\lambda, \phi)$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline953}%
$u, v, h$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1900}%
$\displaystyle u'$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1902}%
$\displaystyle u_{0}b(x)b(x_{e}-x)e^{4/x_{e}},$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1903}%
$\displaystyle v'$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1905}%
$\displaystyle 0,$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1906}%
$\displaystyle h'$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1908}%
$\displaystyle h_{0} - \frac{a}{g}\int _{-\pi/2}^{\phi '}
\left(2\Omega \sin \tau + \frac{u'(\tau)\tan \tau}{a}\right)
u'(\tau)\Dd \tau.$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmldisplayA{displaymath765}%
\begin{displaymath}
  b(x) = \left\{
\begin{array}{lc}
0 & x\le 0 \\
e^{-x^{-1}} & 0 < x 
\end{array}
\right.
\end{displaymath}%
\lthtmldisplayZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmldisplayA{displaymath766}%
\begin{displaymath}
 x = x_{e}\frac{\phi ' - \phi _{b}}{\phi _{e}-\phi_{b}}
\end{displaymath}%
\lthtmldisplayZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1914}%
$\displaystyle \sin \phi '$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1916}%
$\displaystyle \sin \phi \cos \alpha - \cos \alpha \cos \lambda \sin \alpha,$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1917}%
$\displaystyle \sin \lambda '\cos \theta '$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1919}%
$\displaystyle \sin \lambda \cos \phi$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline961}%
$\lambda '$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmldisplayA{displaymath767}%
\begin{displaymath}
  \lambda ' = \left\{
\begin{array}{lc}
\lambda '_{p} & \cos \alpha \cos \lambda \cos \phi + \sin \alpha \sin \phi \ge 0 \\
\pi - \lambda '_{p} & \cos \alpha \cos \lambda \cos \phi + \sin \alpha \sin \phi < 0
\end{array}
\right.
\end{displaymath}%
\lthtmldisplayZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline963}%
$\lambda '_{p}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1926}%
$\displaystyle v\cos \phi$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1928}%
$\displaystyle - u'\sin \alpha \sin \lambda ',$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1929}%
$\displaystyle u\cos \lambda$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1931}%
$\displaystyle v\sin \phi \sin \lambda + u'\cos \lambda '.$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline971}%
$h'$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmldisplayA{displaymath369}%
\begin{displaymath}
  f = 2\Omega(-\cos \lambda \cos \phi \sin \alpha + \sin \phi \cos \alpha)
\end{displaymath}%
\lthtmldisplayZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline977}%
$0, \quad \pi/3$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline989}%
$\phi _{b}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline991}%
$-pi/6$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline993}%
$\phi _{e}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline995}%
$pi/2$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline997}%
$x _{e}   $%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

\stepcounter{subsection}
{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1995}%
$\displaystyle F_{u}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1997}%
$\displaystyle \DD{\tilde{u}}{t} - \frac{\tilde{u}\tilde{v}\tan \phi}{a}
- f \tilde{v} + \frac{g}{a\cos \phi}\DP{\tilde{h}}{\lambda},$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1998}%
$\displaystyle F_{v}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2000}%
$\displaystyle \DD{\tilde{v}}{t} + \frac{\tilde{u}\tilde{v}\tan \phi}{a}
+ f \tilde{v} + \frac{g}{a}\DP{\tilde{h}}{\lambda},$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2001}%
$\displaystyle F_{h}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2003}%
$\displaystyle \DD{\tilde{h}}{t} + \frac{\tilde{h}}{a\cos \phi}
\left[\DP{\tilde{u}}{\lambda} + \DP{\tilde{v}\cos \phi}{\phi}
\right]$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmldisplayA{displaymath768}%
\begin{displaymath}
\DD{}{t} = \DP{}{t} + \frac{u}{a\cos \phi}\DP{}{\lambda} + 
           \frac{v}{a}\DP{}{\phi} 
\end{displaymath}%
\lthtmldisplayZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1001}%
$F_{\zeta}, F_{D}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2007}%
$\displaystyle F_{\zeta}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2009}%
$\displaystyle \frac{1}{a(1-\mu ^{2})}\DP{(F_{v}\cos \phi)}{\lambda} - \frac{1}{a}\DP{(F_{u}\cos \phi)}{\mu},$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2010}%
$\displaystyle F_{D}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2012}%
$\displaystyle \frac{1}{a(1-\mu ^{2})}\DP{(F_{u}\cos \phi)}{\lambda} + \frac{1}{a}\DP{(F_{v}\cos \phi)}{\mu}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1003}%
$\tilde{u}, \tilde{v}, \tilde{h}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2015}%
$\displaystyle \tilde{u}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2017}%
$\displaystyle \overline{u} - \frac{1}{a}\DP{\overline{\psi}}{\phi},$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2018}%
$\displaystyle \tilde{v}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2020}%
$\displaystyle \frac{1}{a\cos \phi}\DP{\overline{\psi}}{\lambda},$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2021}%
$\displaystyle \tilde{h}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2023}%
$\displaystyle \overline{h} + \frac{f}{g}\overline{\psi}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2025}%
$\displaystyle \overline{u}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2027}%
$\displaystyle u_{0}\sin ^{14}(2\phi),$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2028}%
$\displaystyle \overline{h}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2030}%
$\displaystyle h_{0} - \frac{a}{g}\int _{-\pi/2}^{\phi}
\left(2\Omega \sin \tau + \frac{\overline{u}(\tau)\tan \tau}{a}\right)
\overline{u}(\tau)\Dd \tau,$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2031}%
$\displaystyle \overline{\psi}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2033}%
$\displaystyle \psi _{0}\exp \left(-\sigma \frac{1-C}{1+C}\right),$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2035}%
$\displaystyle \psi _{0}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2037}%
$\displaystyle -0.03\frac{gh_{0}}{2\Omega \sin (\pi/4)},$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2038}%
$\displaystyle C$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2040}%
$\displaystyle \sin \phi _{0}\sin \phi
+ \cos \phi_{0}\cos \phi
\left(\lambda - \frac{u_{0}}{a}t - \lambda _{0}\right)$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1007}%
$20, \quad 40$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1013}%
$10^{5}/g$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1015}%
$\sigma $%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1017}%
$(12.74244)^{2}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1019}%
$\lambda _{0}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1021}%
$\phi _{0}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1023}%
$\pi/4$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

\stepcounter{subsection}
{\newpage\clearpage
\lthtmldisplayA{displaymath546}%
\begin{displaymath}
  h_{s} = h_{s0} \left(1 - \frac{1}{R}\sqrt{\mbox{min}[R^{2}, (\lambda -\lambda _{c})^{2}+(\phi - \phi _{c})^{2}]}\right)
\end{displaymath}%
\lthtmldisplayZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1027}%
$\alpha =0$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2100}%
$\displaystyle u_{0}\cos \phi,$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2106}%
$\displaystyle h_{0} - \left(a\Omega u_{0} + \frac{u_{0}^{2}}{2}\right)
(\sin \phi)^{2}/g.$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2110}%
$\displaystyle -u_{0}a\sin \theta,$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2117}%
$\displaystyle \frac{2u_{0}}{a}\sin \theta,$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1035}%
$h_{s0}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1039}%
$\pi$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1047}%
$\pi/6$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

\stepcounter{subsection}
{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2179}%
$\displaystyle -a^{2}\omega \sin \phi + a^{2}K\cos ^{R}\phi \cos R\lambda,$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2182}%
$\displaystyle 0.$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2186}%
$\displaystyle a\omega \cos \phi + aK\cos ^{R-1}\phi (R\sin ^{2}\phi - \cos ^{2}\phi)\cos R\lambda,$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2189}%
$\displaystyle -aKR\cos ^{R-1}\phi \sin \phi \sin R\lambda$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2193}%
$\displaystyle 2\omega\sin \phi - K\sin \phi \cos ^{R}\phi (R^{2}+3R+2)\cos R\lambda,$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmldisplayA{displaymath616}%
\begin{displaymath}
 h = h_{0} + [a^{2}A(\phi) + a^{2}B(\phi)\cos R\lambda +a^{2}C(\phi)\cos 2R\lambda]/g
\end{displaymath}%
\lthtmldisplayZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2200}%
$\displaystyle A(\phi)$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2202}%
$\displaystyle \frac{\omega}{2}(2\Omega + \omega)\cos^{2} \phi$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2203}%
$\displaystyle + \frac{1}{4}K^{2}\cos ^{2R}[(R+1)\cos^{2}\phi
+ (2R^{2} - R - 2) - 2R^{2}cos^{-2}\phi],$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2204}%
$\displaystyle B(\phi)$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2206}%
$\displaystyle \frac{2(\Omega + \omega)K}{(R+1)(R+2)}\cos ^{R}\phi
[(R^{2} + 2R +2) - (R + 1)^{2}\cos ^{2}\phi],$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2207}%
$\displaystyle C(\phi)$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay2209}%
$\displaystyle \frac{1}{4}K^{2}\cos ^{2R}\phi[(R + 1)\cos ^{2}\phi - (R + 2)]$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1055}%
$\omega$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1057}%
$7.848\times 10^{-6}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1061}%
$K$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

\stepcounter{section}
{\newpage\clearpage
\lthtmldisplayA{displaymath769}%
\begin{displaymath}
 \mbox{spmodel@gfd-dennou.org}
\end{displaymath}%
\lthtmldisplayZ
\lthtmlcheckvsize\clearpage}


\end{document}
