Reflection of a Point Disturbance From a Conducting Wall in Two Dimensional Magn
Reflection of a Point Disturbance From a Conducting Wall in Two Dimensional Magn
H Weitzner
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^ IPzill . |!h_ (, _5)(p_p) . .. . So that to leading order and by use of (32) we find /+2s(l, p), -. (P-P) =M 3s^l, p) ^^Q^^-^) • -^ ^P 9s (l, p) Now for j = 3 or 4 and p positive imaginary, s. (l, p)/ — ^^^^ is J op positive imaginary. Hence, if x(p) is increasing as Im (p) in- creases, then the root of h(x, y, t, p) near p is pure imaginary for X > X and has non— zero real part for x
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