The Dipole Field in An Inhomogeneous Atmosphere

Cover The Dipole Field in An Inhomogeneous Atmosphere
The Dipole Field in An Inhomogeneous Atmosphere
Bernard Friedman
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In other words, t is en eigenvalue and w (r) is an elgenf ijnction of the following ^ *J problem: rind th« values of t for which T(r), the solution of the following differential equation: (3M -^ * P - i^1 (rr) . , dr r •' is regular at r » and satisfies the radiation condition (I5) at infinity, that is, Itm I dCrr) . , 1 .
^ —J — ^ - Ik rr « r->oo' dr ' Pttt (35) P =/ w^ (r)^ 4r J ^ J 1/2 so that w (r)^, i" a noraaliied eigenfunction of (3^); then the residue given tj J Ijy (32) will be shown t
...o be equal to -20u (36) w Cb) w (r) P (-C08 ©) eln IT t, 2 pj ... .. . J This resnlt will be obtnined from a consideration of the following two eqijAtlone: d^Crv^) t(t+l) 1 t. (t +1).
_J — J dr^ d^nr, ) ] = dr ■] (iv^ ) =0 .
Here t hee any valiie and Is not an eigenTalne, Mnltiply the first equation by rw, the second by rr subtract and integrate with respect to r from to oo.
We obtain 07) (t-t )(t+t -t-l) /oo J dr = nr^ f? ^^t.^ " "'t, d? ^"t^ 00 Notice the term at «ero drops out because by ceflnition ▼.


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