Table 1: $\displaystyle \left. \frac{\tau_{\rm Joule}}{\tau_{\rm visc}} \right\vert _{A.w. ({\parallel}) \atop {\rm f.ms.w.} ({\parallel})}$ calculated for $B_0 = 10; 50; 100~\mbox{G}$ in the corona.
  $T = 10^{5} \mbox{ K}$ $T = 5 \times 10^{5} \mbox{ K}$ $T = 10^{6} \mbox{ K}$
  0.0063 0.0315 0.063
$n = 10^{8} \hspace*{1mm}\mbox{cm$^{-3}$ }$ 0.000252 0.00126 0.00252
  0.000063 0.000315 0.00063
  0.63 3.15 6.3
$n = 10^{10} \hspace*{1mm} \mbox{cm$^{-3}$ }$ 0.0252 0.126 0.252
  0.0063 0.0315 0.063
  63 315 630
$n = 10^{12} \hspace*{1mm} \mbox{cm$^{-3}$ }$ 2.52 12.6 25.2
  0.63 3.15 6.3


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