Transcendental Equations in Electromagnetic Theory

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Transcendental Equations in Electromagnetic Theory
Leon Kotin
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Then lim l(|)"V(v)| =lime-^l°Sx/2jp(^)| ^ ^ ITCvJI X -^ 0+ ' I ^ where Also c > 1 and V = i^ = 11m v. — o o lim |(|)V(-)e-^^| = lim e- 1°S ^/2 . P« \r{-. )\ = ^ e^^'' iPC-v^)!
Since v =16, If^Cv )| = IF^C-v )l: and since Er(x) = in the limit also, o o I ' ^ o I I ' o I ' V 6 rt/2 _^ ^^ ^^/^ the tn/o limits above miost be equal, whence c = e = lim e ^ ' .
6. The derivative of v We can obtain some interesting results not only for small x, as in the dv last section, but for any x by examining -t—
.... However, it is not much more difficult to consider complex values of the argument. W. E shall derive a formula which was first obtained by Watson (see [5], p- ^08), ^ = 2c I K (2c sinh t) e'^^^ dt, dv jo o^ . ' where v is real and c is a positive zero (in z) of the cylindrical function J (z) cos s + Y (z) sin s for constant s. This form immediately excludes H .
V/e shell generalize it to apply to complex values of z and v, as well as to any function of the form C (z) = c, J (z) + c_Y (z), where c, and c^ are independent V 1 v^ 2 V 1 2 ^ of both z and v.


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