Effects of thermal conduction and compressive viscosity on the period ratio of the slow mode

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Table 2:

Values of the compressive viscosity parameter $\epsilon$ .
T₀ (MK)	$\epsilon$ (2L=50 Mm)	$\epsilon$ (2L=100 Mm)	$\epsilon$ (2L=200 Mm)	$\epsilon$ (2L=300 Mm)	$\epsilon$ (2L=400 Mm)
1	0.883e-3	0.442e-3	0.221e-3	0.147e-3	0.110e-3
2	0.707e-2	0.353e-2	0.177e-2	0.118e-2	0.883e-3
3	0.239e-1	0.119e-1	0.596e-2	0.398e-2	0.298e-2
4	0.565e-1	0.283e-1	0.141e-1	0.942e-2	0.707e-2
5	0.110	0.552e-1	0.276e-1	0.184e-1	0.138e-1
6	0.191	0.954e-1	0.477e-1	0.318e-1	0.239e-1
7	0.303	0.152	0.758e-1	0.505e-1	0.379e-1
8	0.452	0.226	0.113	0.754e-1	0.565e-1
9	0.644	0.322	0.161	0.107	0.805e-1
10	0.883	0.442	0.221	0.147	0.110

Notes. Variations in the compressive viscosity parameter $\epsilon$ with changes in temperature T₀ for different loop lengths 2L. Again the loop pressure is p₀=0.55 Pa and the other parameters are as in Table 1. The compressive viscosity is $\nu_0=10^{-17}$ in mks units.

Source LaTeX | All tables | In the text

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