Table 2: $\displaystyle \left . f_{\rm c}^{\rm Joule} \right \vert _{ A.w. ({\parallel }) \atop {\rm f.ms.w.} ({\parallel }, {\perp })}$ calculated for $B_0 = 10; 50; 100~\mbox{G}$ in the corona.
$T = 10^{5} \mbox{ K}$ $T = 5 \times 10^{5} \mbox{ K}$ $T = 10^{6} \mbox{ K}$

$2.74 \times 10^{10}$ $2.68 \times 10^{11}$ $7.20 \times 10^{11}$

$n = 10^{8} \hspace{1mm}\mbox{cm$^{-3}$ }$ $6.85 \times 10^{11}$ $6.71 \times 10^{12}$ $1.80 \times 10^{13}$

$2.74 \times 10^{12}$ $2.68 \times 10^{13}$ $7.20 \times 10^{13}$

$3.17 \times 10^{8}$ $3.04 \times 10^{9}$ $8.12 \times 10^{9}$

$n = 10^{10} \hspace{1mm} \mbox{cm$^{-3}$ }$ $7.92 \times 10^{9}$ $7.61 \times 10^{10}$ $2.03 \times 10^{11}$

$3.17 \times 10^{10}$ $3.04 \times 10^{11}$ $8.12 \times 10^{11}$

$3.75 \times 10^{6}$ $3.51 \times 10^{7}$ $9.30 \times 10^{7}$

$n = 10^{12} \hspace{1mm} \mbox{cm$^{-3}$ }$ $9.39 \times 10^{7}$ $8.79 \times 10^{8}$ $2.32 \times 10^{9}$

$3.75 \times 10^{8}$ $3.51 \times 10^{9}$ $9.30 \times 10^{9}$

**Table 2:** $\displaystyle \left . f_{\rm c}^{\rm Joule} \right \vert _{ A.w. ({\parallel }) \atop {\rm f.ms.w.} ({\parallel }, {\perp })}$ calculated for $B_0 = 10; 50; 100~\mbox{G}$ in the corona.
	$T = 10^{5} \mbox{ K}$	$T = 5 \times 10^{5} \mbox{ K}$	$T = 10^{6} \mbox{ K}$
	$2.74 \times 10^{10}$	$2.68 \times 10^{11}$	$7.20 \times 10^{11}$
$n = 10^{8} \hspace{1mm}\mbox{cm$^{-3}$ }$	$6.85 \times 10^{11}$	$6.71 \times 10^{12}$	$1.80 \times 10^{13}$
	$2.74 \times 10^{12}$	$2.68 \times 10^{13}$	$7.20 \times 10^{13}$
	$3.17 \times 10^{8}$	$3.04 \times 10^{9}$	$8.12 \times 10^{9}$
$n = 10^{10} \hspace{1mm} \mbox{cm$^{-3}$ }$	$7.92 \times 10^{9}$	$7.61 \times 10^{10}$	$2.03 \times 10^{11}$
	$3.17 \times 10^{10}$	$3.04 \times 10^{11}$	$8.12 \times 10^{11}$
	$3.75 \times 10^{6}$	$3.51 \times 10^{7}$	$9.30 \times 10^{7}$
$n = 10^{12} \hspace{1mm} \mbox{cm$^{-3}$ }$	$9.39 \times 10^{7}$	$8.79 \times 10^{8}$	$2.32 \times 10^{9}$
	$3.75 \times 10^{8}$	$3.51 \times 10^{9}$	$9.30 \times 10^{9}$

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