Abstract
The redistribution of charged particles in the mirror field B(s, t) = B0T(t){1 + [s/a(t)]v (t)}is worked out for slow changes in T(t), a(t), and v(t). It is found that increasing T(t) gives a relatively greater particle density increase in the center of the field than deep in the mirrors s≫a(t). The mirror distance retracts like 1/T1/(v+2). Decreasing a(t) has the opposite effect. Field variations constrained to preserve T(t) a2(t) and v(t) leave the form of the particle distribution unchanged, increasing the density everywhere by the same factor.
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