All Figures

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig1.eps}\end{figure}$ Figure 1: FAL heating rates per unit volume, and per unit mass as a function of z. The dashed line denotes a negative heating rate. The units of the heating rate per unit mass are 10⁹ erg g^-1 s^-1.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig2.eps}\end{figure}$ Figure 2: Electron, proton, proxy ion, H, and He I number densities, temperature, and proxy ion mass as functions of z. The temperature is given in units of 500 K. The proxy ion mass is given in units of three times the proton mass.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig3.eps}\end{figure}$ Figure 3: Area averaged heating rates per unit volume, weighted by filling factor, and the FAL heating rate per unit volume as functions of z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig4.eps}\end{figure}$ Figure 4: Area averaged heating rates per unit mass, weighted by filling factor, and the FAL heating rate per unit mass as functions of z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig5.eps}\end{figure}$ Figure 5: Electron, proton, proxy ion, and effective ion magnetizations averaged over the areas defined by $0 \leq R \leq R_0$ (denoted by R₀) and $R_0 \leq R \leq 2 R_0$ (denoted by R₀ - 2 R₀) as functions of z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig6.eps}\end{figure}$ Figure 6: Efficiency of Pedersen current dissipation as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig7.eps}\end{figure}$ Figure 7: Ratio of parallel to Pedersen conductivity as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig8.eps}\end{figure}$ Figure 8: Heating rate per unit volume as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig9.eps}\end{figure}$ Figure 9: Heating rate per unit mass as a function of R and z, multiplied by the filling factor f=0.02.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig10.eps}\end{figure}$ Figure 10: Ratio of Pedersen current dissipation rate to parallel current dissipation rate, averaged over areas with radii of R₀ and 2 R₀, as functions of z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig11.eps}\end{figure}$ Figure 11: Magnitude of the component of the CM electric field that is perpendicular to ${\vec B}$ as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig12.eps}\end{figure}$ Figure 12: Magnitude of the component of the electric field that is parallel to ${\vec B}$ as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig13.eps}\end{figure}$ Figure 13: Parallel conductivity as a function of z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig14.eps}\end{figure}$ Figure 14: Pedersen conductivity as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig15.eps}\end{figure}$ Figure 15: Magnitude of the Hall conductivity as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig16.eps}\end{figure}$ Figure 16: Ratio of the magnitudes of the effective ion and electron Pedersen current densities as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=10.9cm,clip]{fig17.eps}\end{figure}$ Figure 17: Ratio of the magnitudes of the proton and proxy ion Pedersen current densities as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=10.9cm,clip]{fig18.eps}\end{figure}$ Figure 18: Current density parallel to ${\vec B}$ as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig19.eps}\end{figure}$ Figure 19: Magnitude of Pedersen current density as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig20.eps}\end{figure}$ Figure 20: Magnitude of Hall current density as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig21.eps}\end{figure}$ Figure 21: Pressure and number density as functions of R at z=0. The pressure is given in units of 10⁵ dynes cm^-2. The number density is given in units of 10¹⁷ cm^-3.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig22.eps}\end{figure}$ Figure 22: Magnitude of the flow velocity perpendicular to ${\vec B}$ as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig23.eps}\end{figure}$ Figure 23: Magnitude of the flow velocity parallel to ${\vec B}$ as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig24.eps}\end{figure}$ Figure 24: Magnitude of the convection electric field as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig25.eps}\end{figure}$ Figure 25: Magnitude of the component of ${\vec E}$ perpendicular to ${\vec B}$ as a function of R and z.
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In the text

$\begin{figure} \par\includegraphics[width=11cm,clip]{fig26.eps}\end{figure}$ Figure 26: Ratio of the magnitudes of the convection electric field and ${\vec E}_\perp$ as a function of R and z.
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In the text