Figure 12.
Growth rate of the toroidal mode as a function of Ma. The four panels refer to different values of the pitch parameter Pc (Top left: Pc = 10; Top right: Pc = 1; Bottom left: Pc = 0.1; Bottom right: Pc = 0.01). The solid curves are for α = 1, dashed curves are for α = 0.2, curves with different colours refer to different values of γc = 1.01, 2, 5, 10 as indicated in the legend of each panel. The black lines represent the growth rate calculated with non-relativistic ideal MHD equations at zero thermal pressure and the same pitch and α in the respective panel. If the dashed curve is absent in any panel, this means that the equilibrium with α = 0.2 is not possible for that pair of Pc and γc associated with this panel. The wavenumber is k = 0.01 in all the cases, although the growth rate is essentially independent of this value.

Growth rate of the toroidal mode as a function of Ma. The four panels refer to different values of the pitch parameter Pc (Top left: Pc = 10; Top right: Pc = 1; Bottom left: Pc = 0.1; Bottom right: Pc = 0.01). The solid curves are for α = 1, dashed curves are for α = 0.2, curves with different colours refer to different values of γc = 1.01, 2, 5, 10 as indicated in the legend of each panel. The black lines represent the growth rate calculated with non-relativistic ideal MHD equations at zero thermal pressure and the same pitch and α in the respective panel. If the dashed curve is absent in any panel, this means that the equilibrium with α = 0.2 is not possible for that pair of Pc and γc associated with this panel. The wavenumber is k = 0.01 in all the cases, although the growth rate is essentially independent of this value.

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