I. Introduction
Applications of condensed liners [1]–[7] in high-energy-density physics need the liners' velocities of about 1 and more. To achieve such velocities, the megagauss-range magnetic fields are needed, which cause melting and even evaporation and transition to plasma of some part of the liner (the skin layer) [8] and, consequently, to the loss of strength in this part of the liner and the development of Rayleigh–Taylor (RT) and sausage instabilities. As a result, in this part, the conditions for RT and sausage instabilities are provided. This instability development may result in inhomogeneous state of the liner, spoiling the conditions of its utilization or even leading to its destruction.