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% !!! IMAGES START HERE !!!

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$ T=150$%
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{\newpage\clearpage
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$ p=400$%
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$ 5.0 \times 10^{8}$%
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$ ^{-1}$%
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$ u$%
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$ w$%
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$ \theta$%
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$ \Pi$%
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$ \rho_s$%
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$ p$%
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$ T$%
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$\displaystyle \theta$%
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$\displaystyle \equiv$%
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$\displaystyle T \left( \frac{p_0}{p} \right)^{\frac{R}{c_p}},
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$\displaystyle \Pi$%
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$\displaystyle \left( \frac{p}{p_0} \right)^{\frac{R}{c_p}} =
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$ p_0$%
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$ R$%
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$ c_p$%
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$ R \simeq 188.9$%
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$ c_p \simeq
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$ p_0 = 700$%
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$ \phi$%
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$ \overline{\phi}$%
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$ \phi^{\prime}$%
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$\displaystyle =$%
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$\displaystyle u^{\prime}(x,z,t), \Deqlab{ZA}$%
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$ ^{\prime}$%
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$\displaystyle \DP{\overline{p}}{z} = - \overline{\rho} g \Deqlab{hydrostat1}$%
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$ g$%
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$ \overline{\Pi}$%
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$ \overline{\theta}$%
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$ _2$%
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$\displaystyle - u \DP{u}{x} - w \DP{u}{z} - c_p \overline{\theta}
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$\displaystyle - u \DP{w}{x} - w \DP{w}{z} - c_p \overline{\theta}
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\frac{\theta^{\prime}}{\overline{\theta}}, \Deqlab{AB}$%
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$\displaystyle - u \DP{\theta^{\prime}}{x} - w \DP{\theta^{\prime}}{z}
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{\newpage\clearpage
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$\displaystyle - \frac{\overline{c}^2}{c_p \overline{\rho} \overline{\theta}^2}
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- \frac{\overline{c}^2}{c_p \overline{\rho} \overline{\theta}^2}
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$\displaystyle - \DP{(\rho_s u)}{x} - \DP{(\rho_s w)}{z}
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$ \overline{c}$%
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$\displaystyle {\overline{c}}^2  = \frac{c_p}{c_v} R \overline{T} = \frac{c_p}{c_v} R \overline{\theta} \overline{\Pi}. \Deqlab{Sound}$%
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$ c_v$%
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$ c_v \simeq 545.2$%
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$ D_u$%
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$ D_w$%
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$ D_{\theta}$%
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$ D_{\rho_s}$%
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$ Q_{cond}$%
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$ Q_{rad}$%
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$ Q_{dis}$%
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$ M_{cond}$%
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$ M_{fall}$%
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$\displaystyle Q_{cond} = \frac{L M_{cond}}{c_p \overline{\rho}} \Deqlab{AF}$%
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$ L$%
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$ L \simeq 5.86 \times 10^5$%
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$\displaystyle \frac{\overline{c}^2}{c_p \overline{\theta}^2}
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$\displaystyle \frac{\overline{c}^2}{c_p \overline{\theta}^2}
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$\displaystyle \frac{\overline{c}^2 L }
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M_{cond}
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( Q_{rad} + Q_{dis} )
\Deqlab{AG}$%
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{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1526}%
$\displaystyle - \frac{\overline{c}^2}{c_p \overline{\rho} \overline{\theta}^2}
\left[ \DP{ (\overline{\rho} \overline{\theta} u) }{x}
+ \DP{ (\overline{\rho} \overline{\theta} w) }{z} \right]$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1530}%
$\displaystyle + \frac{\overline{c}^2}{c_p \overline{\rho} \overline{\theta}}
\left( \frac{L}{c_p \overline{T}} - 1 \right) M_{cond}
+ \frac{\overline{c}^2}{c_p \overline{\theta}^2 \overline{\Pi}}
( Q_{rad} + Q_{dis} ).
\Deqlab{AH}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1532}%
$ O(\overline{T}) \sim 150$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1544}%
$ L / (c_p \overline{T}) > 1 $%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1554}%
$\displaystyle \phi(x,z,t) = \phi(x+L,z,t) \Deqlab{BoundaryA}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1556}%
$ D$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1560}%
$ \psi$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1565}%
$\displaystyle w$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1569}%
$\displaystyle 0, \quad \quad (z = 0, D) \Deqlab{boundaryB}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1573}%
$\displaystyle \DP{\psi}{z}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1577}%
$\displaystyle 0, \quad \quad (z = 0, D) \Deqlab{boundaryC}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

\stepcounter{section}
\stepcounter{subsection}
{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1590}%
$ D_\theta$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1597}%
$\displaystyle D_u$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1601}%
$\displaystyle - \DP{}{x} \left[ - \frac{2}{3} K_m \DP{u}{x} + \frac{2}{3} E \right]
- \DP{}{x} \left[ - K_m \left( \DP{u}{x} + \DP{w}{z} \right) \right]
, \Deqlab{TurbA}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1605}%
$\displaystyle D_w$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1609}%
$\displaystyle - \DP{}{x} \left[ - K_m \left( \DP{w}{x} + \DP{u}{z} \right) \right]
- \DP{}{z} \left[ - \frac{2}{3} K_m \DP{w}{x} + \frac{2}{3} E \right]
, \Deqlab{TurbB}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1613}%
$\displaystyle D_{\theta}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1617}%
$\displaystyle - \DP{}{x} \left[ K_h \DP{\theta^{\prime}}{x} \right]
- \DP{}{z} \left[ K_h \DP{(\theta^{\prime} + \overline{\theta})}{z}
\right], \Deqlab{TurbC}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1621}%
$\displaystyle D_{\rho_s}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1625}%
$\displaystyle - \DP{}{x} \left[ K_h \DP{\rho_s}{x} \right]
- \DP{}{z} \left[ K_h \DP{\rho_s}{z}  \right] \Deqlab{TurbD}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1627}%
$ K_m$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1629}%
$ K_h$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1631}%
$ E$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1639}%
$\displaystyle E = \left( \frac{K_m}{C_m l} \right)^2 \Deqlab{TurbE}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1641}%
$ l$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1643}%
$ \Delta x$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1645}%
$ \Delta z$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1647}%
$ l = (\Delta x \Delta z)^{1/2}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1649}%
$ C_m$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1655}%
$\displaystyle K_h = 3 K_m \Deqlab{TurbF}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1660}%
$\displaystyle \DP{K_m}{t}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1664}%
$\displaystyle - \left( u \DP{K_m}{x} + w \DP{K_m}{z} \right)
- \frac{3 g {C_m}^2 l^2}{2 \overline{\theta}}
\DP{\theta^{\prime}}{z}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1666}%
$\displaystyle + {C_m}^2 l^2 \left[ \left( \DP{u}{x} \right)^2 + \left( \DP{w}{z}
\right)^2 \right]
+ \frac{{C_m}^2 l^2}{2} \left( \DP{u}{z} + \DP{w}{x} \right)^2$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1668}%
$\displaystyle - \frac{K_m}{3} \left( \DP{u}{x} + \DP{w}{z} \right)
+ \Dinv{2} \left( \DP[2]{{K_m}^2}{x} + \DP[2]{{K_m}^2}{z} \right)$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1672}%
$\displaystyle + \left( \DP{K_m}{x} \right)^2 + \left( \DP{K_m}{z} \right)^2
- \frac{C_{\varepsilon}}{2 C_m l^2} {K_m}^2.
\Deqlab{TurbG}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1674}%
$ C_{\varepsilon}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1676}%
$ C_m = C_{\varepsilon}
= 0.2$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1682}%
$\displaystyle Q_{dis}  = \frac{C_{\varepsilon}}{c_p l} E^{3/2}  = \frac{C_{\varepsilon}}{c_p l} \left( \frac{K_m}{C_m l} \right)^3  \Deqlab{TurbH}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

\stepcounter{subsection}
{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1688}%
$ F_h$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1692}%
$\displaystyle F_h = c_D V_{lowest} (T_{gnd} - T_{lowest}) / \Delta z \Deqlab{TurbI}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1694}%
$ c_D$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1696}%
$ V_{lowest}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1698}%
$ T_{gnd}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1700}%
$ T_{lowest}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1702}%
$ c_D = 1.5 \times 10^{-3}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1706}%
$\displaystyle V_{sfc} = \sqrt{u_{lowest}^2 + u_0^2} \Deqlab{TurbJ}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1708}%
$ u_{lowest}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1710}%
$ u_0$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1716}%
$ u_0 = 3.0$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

\stepcounter{section}
{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1735}%
$ \mu$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1748}%
$\displaystyle M_{cond} = \frac{4 \pi r_d \overline{\rho} N^{*}}{R_h} (S - 1).   \Deqlab{CloudB}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1750}%
$ R_h$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1752}%
$ S$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1754}%
$ r_d$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

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

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1763}%
$\displaystyle \frac{L^2}{k R T^2} = \frac{L^2}{k R \theta^2 \Pi^2},
\Deqlab{CloudC}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1767}%
$\displaystyle S$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1771}%
$\displaystyle \frac{p}{p_{\ast}} = \frac{{p_0}^{\frac{c_p}{R}} \Pi}{p_{\ast}}
\Deqlab{CloudE}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1775}%
$\displaystyle r_d$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1779}%
$\displaystyle \left(
r_d^3 + \frac{3 \rho_s}{4 \rho_I \pi \overline{\rho} N^{*}}
\right)^{1/3}
\Deqlab{CloudA}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1781}%
$ k$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1783}%
$ p_{\ast}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1787}%
$ \rho_I$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1793}%
$ r_{aero}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1795}%
$ N^{*}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1797}%
$ \rho_I = 1.565 \times 10^3$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1799}%
$ ^3$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1809}%
$\displaystyle p_{\ast} \simeq \exp \left( A - \frac{B}{T} \right)  \Deqlab{CloudG}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1811}%
$ A$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1813}%
$ B$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1817}%
$ A =
27.4$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1819}%
$ B = 3103$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1825}%
$ V_{term}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1829}%
$\displaystyle M_{fall} = \DP{}{z} \left( \rho_s V_{term} \right) \Deqlab{CloudI}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1835}%
$\displaystyle V_{term} = C_{sc} \frac{2 r_d^2 g \rho_I}{9 \eta} \Deqlab{CloudJ}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1837}%
$ C_{sc}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1841}%
$\displaystyle C_{sc} = 1 + 1.255 \frac{\lambda}{r_d} \Deqlab{CloudK}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1843}%
$ \lambda$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1849}%
$\displaystyle \lambda = \frac{k_B T}{\sqrt{2} \pi \sigma^2 p} \Deqlab{CloudL}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1851}%
$ k_B$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1853}%
$ \sigma$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1857}%
$ k_B =
1.38 \times 10^{-23}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1859}%
$ ^2$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1861}%
$ ^{-2}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1865}%
$ \sigma =
3.3 \times 10^{-10}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1867}%
$ \eta$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay1871}%
$\displaystyle \eta = \eta_{ref} \left( \frac{T_{ref} + C_{CO_2}}{T + C_{CO_2}} \right)  \left( \frac{T}{T_{ref}} \right)^{3/2} \Deqlab{CloudM}$%
\lthtmlindisplaymathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1873}%
$ \eta_{ref}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1875}%
$ T_{ref}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1877}%
$ C_{CO_2}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1881}%
$ \eta_{ref} = 1.47 \times
10^{-5}$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1883}%
$ \cdot$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1885}%
$ T_{ref} = 293$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline1887}%
$ C_{CO_2} = 240$%
\lthtmlinlinemathZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlfigureA{figure505}%
\begin{figure} \begin{center}
\Depsf[][][width=6.0cm,angle=270]{ps/radius-dens.ps}
  
 \end{center}
  \end{figure}%
\lthtmlfigureZ
\lthtmlcheckvsize\clearpage}

{\newpage\clearpage
\lthtmlfigureA{figure513}%
\begin{figure} \begin{center}
\Depsf[][][width=6.0cm,angle=270]{ps/Vterm.ps}
  
 \end{center}
  \end{figure}%
\lthtmlfigureZ
\lthtmlcheckvsize\clearpage}


\end{document}
