In order to investigate the influences of ballooning modes with moderate wave numbers on MHD equilibrium, fully three-dimensional nonlinear MHD simulations with or without a large parallel thermal conductivity kappa(parallel to) are carried out for a fairly Mercier-unstable low-beta MHD equilibrium in the inward-shifted Large Helical Device (LHD) configuration, which is considered to be avoided by pressure profile control in experiments. In the case without a kappa(parallel to) corresponding to a nearly non-dissipative plasma, such ballooning modes are so dangerous that a pressure collapse occurs in the core region and the plasma expands beyond the outermost flux surface. On the other hand, pressure deformation is limited in the core region for the case with a large kappa(parallel to), because ballooning modes with moderate wave numbers are significantly suppressed by kappa(parallel to). Since the core pressure collapse in a low-beta plasma will become an obstacle on the way to attaining a high-beta plasma in experiments, the operation regime or pressure profile in the inward-shifted LHD configuration might be restricted, at the least low-beta regime, which is consistent with the experimental observation.
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