The marginal stability of MHD modes is discussed in application for high be
ta multiple mirror experiments planned at Budker Institute of Nuclear Physi
cs. Flute modes are dangerous in axisymmetric systems with beta < 1. In the
case of "wall confined" plasmas, (beta much greater than 1), pressure slig
htly varies along the radius providing less radial gradient and more stabil
ity against MHD modes. Effect of ion-ion viscosity becomes important in cor
rugated magnetic field. It results in the reduction of the growth rate by a
factor beta(1/2). Il, the process of start up and plasma heating beta < 1.
If flute modes are stabilized during this period by the line-tying mechani
sm ballooning modes are still unstable when beta > beta(cr). A. very low ba
llooning margin is predicted in multiple mirror with the large number of ce
lls: beta(cr) less than or equal to pi(2) /N-2. For the number of cells N s
imilar or equal to 10: beta(cr) similar or equal to 5%. Results of the calc
ulations are discussed in the context of old and new multiple mirror experi
ments.