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{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline804}%
$\{{\svector x}_{bh}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline806}%
${\svector q}_{bh}\}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline812}%
${\svector x}_b$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline814}%
${\svector x}_{bh}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline816}%
${{\svector x}_h} = ({\svector x}_r - {\svector x}_s)/2$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline818}%
${\svector x}_c = ({\svector x}_r + {\svector x}_s)/2$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline820}%
${\svector p}( {\svector x}_{bh} , {\svector x}_c + {{\svector x}_h} )$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline822}%
${\svector p}( {\svector x}_{bh} , {\svector x}_c - {{\svector x}_h} )$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1490}%
$\displaystyle \max_{{\svector {\scriptstyle x}}_c}
~ \Bigl \|
[{\svector p}( {\svector x}_{bh} , {{\svector x}_c} - {{\svector x}_h} ) 
+{\svector p}( {\svector x}_{bh} , {{\svector x}_c} + {{\svector x}_h} )] 
\cdot {\svector q}_{bh}
\Bigr \|
$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1492}%
$\displaystyle {\svector p}( {\svector x}_{bh} , {{\svector x}_c} - {{\svector x}_h} )
+{\svector p}( {\svector x}_{bh} , {{\svector x}_c} + {{\svector x}_h} )
= 2   ~ P ({\svector x}_{bh}) ~ \cos ( \theta_{cbh} / 2) ~
{\svector q}_{bh} ,$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1493}%
$\displaystyle \mbox { where } \cos ( \theta_{cbh} ) \equiv
[ {\svector p}( {\svector x}_{bh} , {{\svector x}_c} - {{\svector x}_h} ) \cdot
{\svector p}( {\svector x}_{bh} , {{\svector x}_c} + {{\svector x}_h} ) ] / P ( {\svector x}_{bh} )^2 .$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline824}%
$\theta_{cbh}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1496}%
$\displaystyle t_{ch} ({\svector x}_{bh}) = T({\svector x}_{bh} , {{\svector x}_c} - {{\svector x}_h} ) + T({\svector x}_{bh} , {{\svector x}_c} + {{\svector x}_h} ) .
$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline828}%
${{\svector x}_c} $%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline830}%
$t_{ch}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline834}%
${\svector p}_{ch} = {\svector {\nabla}}_{{\svector {\scriptstyle x}}_c} t_{ch} $%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline836}%
${\svector {\nabla}}_{{\svector {\scriptstyle x}}_c} \equiv ({\svector {\nabla}}_{{\svector {\scriptstyle x}}_s} +  {\svector {\nabla}}_{{\svector {\scriptstyle x}}_r})/2 $%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1504}%
$\displaystyle \max_{{\svector {\scriptstyle x}}_{bh}}
~ \Bigl \| 
[ {\svector p}( {{\svector x}_c} - {{\svector x}_h} , {\svector x}_{bh} ) 
+ {\svector p}( {{\svector x}_c} + {{\svector x}_h} , {\svector x}_{bh} ) ]
\cdot {\svector p}_{ch} 
\Bigr \|
$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline838}%
$\{t_{ch},{\svector p}_{ch}\}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline840}%
$\{{\svector x}_{bh}, {\svector q}_{bh}\}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline844}%
$t_{ch} ({\svector x}_{bh})$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

\stepcounter{subsection}
{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1511}%
$\displaystyle \Delta t_{ch} ({\svector x}_{bh}) \equiv 
t_{ch} ({\svector x}_{bh} + \Delta {\svector x}_{bh} ) -
t_{ch} ({\svector x}_{bh} ) 
= 2 P ({\svector x}_{bh} ) \cos ( \theta_{cbh} / 2 ) {\svector q}_{bh} \cdot \Delta
{\svector x}_{bh} .
$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1513}%
$\displaystyle \Delta \hat {\svector x}_{cbh} =
{ \Delta t_{ch} ({\svector x}_{bh}) \over
 2 P ({\svector x}_{bh} ) \cos ( \theta_{cbh} / 2 ) } ~ {\svector q}_{bh} .
$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1515}%
$\displaystyle e_{cbh} \equiv 
{ \Delta t_{ch} ({\svector x}_{bh}) \over
 \cos ( \theta_{cbh} / 2 ) }  .
$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

\stepcounter{subsection}

\end{document}
