1973 Volume 34 Issue 6 Pages 1649-1658
The flow of an electrically conducting viscous fluid past an insulated flat plate at a small incidence, θ, is dealt with by the linearized approximation. The behavior of the flow at large values of viscous Reynolds number, R, magnetic Reynolds number, Rm, and pressure number, S, is studied. Four characteristic types of flow are shown. In the first case: 1<<R≤O(1⁄sinθ) and κ1=(1+Rm⁄R)−[(1−Rm⁄R)2+4RmS⁄R]1⁄2>0, the flow field reduces to the conventional potential flow satisfying the Kutta-Joukowski condition. In the second case: 1<<R≤O(1⁄sinθ) and κ1<0, the flow field becomes the potential flow satisfying the MHD Kutta-Joukowski condition. In the third case: O(1⁄sin2θ)<<R and κ1>0, the flow field consists of a potential field and a wide wake spreading downstream, where the flow is rotational and the velocity almost vanishes. In the last case: O(1⁄sin2θ)<<R and κ1<0, the flow field consists of two wide wakes spreading both up- and downstream.
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