# Full text of "Scientific Papers - Vi"

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1911] PROBLEMS IN THE CONDUCTION OP HEAT 61 In considering the effect of periodic sources distributed over a plane xy, we may suppose v oc cos Ix . cos my, ........................... (59) or again v oc Jn (Icr) . cos nd, ........................... (60) where r2 = x* + yz. In either case if we write I2 + in" = k2, and assume v proportional to eipt, (1) gives dzv/dzz = (k* + ip)v ............................ (61) Thus, if Jc* + ip =.R (cosa + isin a), ....................... (62) where A includes the factors (59) or (60). If the value of v be given on the plane z = 0, that of A follows at once. If the magnitude of the source be given, A is to be found from the value of dvjdz when z = 0. The simplest case is of course that where k = 0. If Veipt be the value of v when z = 0, we find v= Fete*e-Wi»p) ; ............ -. ............... (64) or when realized Vss Ve-Wa»#cos{p*-*V(.p/2)}> ................... (65) corresponding to v= V cos pt when z = 0. From (64) - f — J = *J(ip). 7e*« = \ae[^, ..................(66) if cr be the source per unit of area of the plane regarded as operative in a medium indefinitely extended-in both directions. Thus in terms of o-, v = ^~*i(^e-^^,.........................(67) or in real form ..............(68) •" Yjf corresponding to the uniform source a cos pt In the above formulae z is supposed to be positive. On the other side of the source, where z itself is negative, the signs must be changed so that the terms containing z may remain negative in character. When periodic sources are distributed over the surface of a sphere (radius = c), we may suppose that v is proportional to the spherical surface harmonic Sn. As a function of r and t, v is then subject to (38); and when we introduce the further supposition that as dependent on t, v is proportional to eipt, we have d*(rv) n(n dr* r2 (rv) — ip (rv) = 0................(69)) independently. ndv\ . 1 d*v . , . ,^ rt