Table 1: Values of the constant parameters used in the calculation of our illustrative solutions. The dimension of C isg^1/2 cm $^{(2-3\gamma )/2\gamma }$ /dyn $^{1/2\gamma }$ .
parameter value

p₀₀ 100 dyn/cm²

p₀₁ -70 dyn/cm²

h₀₀ 10⁴ G²

h₀₁ $1.7593\times 10^3$ G²

L_x 15 000 km

L_z $6.5\cdot L_x$ km

C 10^-6

$\gamma$ 5/3

**Table 1:** Values of the constant parameters used in the calculation of our illustrative solutions. The dimension of C isg^1/2 cm $^{(2-3\gamma )/2\gamma }$ /dyn $^{1/2\gamma }$ .
parameter	value
p₀₀	100 dyn/cm²
p₀₁	-70 dyn/cm²
h₀₀	10⁴ G²
h₀₁	$1.7593\times 10^3$ G²
L_x	15 000 km
L_z	$6.5\cdot L_x$ km
C	10^-6
$\gamma$	5/3

Source LaTeX | All tables | In the text

	1 Introduction
	2 Basic equations and equilibrium model
	3 Fast magnetosonic waves
	4 Swing amplification of Alfvén waves
	5 Numerical study of the problem
	6 Discussion
	7 Conclusions
	References