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We consider the motion of an inviscid compressible fluid under the mutual interactions with magnetic field. We show that the initial value problem is ill–posed in the class of weak solutions for a large class of physically admissible data. We also consider the same problem for inviscid heat–conductive fluid and show the same result under certain restrictions imposed on the magnetic field. The main tool is the method of convex integration adapted to the Euler system with `variable coefficients’.

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