X cash ( C B~ COS ej) sink epej. Now making use of modified Bessel and Struve functions of the vth kind, defined respectively as [5] I,(cBj) = 2(cBj/2)' ["' f i q v + $1 0 cosh (cBj cos Sj) sin2' Opej (17) and L,(cBj) = 2(cBj/2)' [":' sinh (,Ej COS S j ) sin" Opej (18) J;;zr(v + 4) where and rearranging, P may be written as Next, consider the case when mj is even. The integral P can be evaluated by first expanding cos m,8, in terms of the powers of sin Sj, and then using (17) and (18); the final result turns out to be Using (20), (21), and (9), the magnitude of the desired frequency component at the output can be obtained. COMPUTATION OF COEFFICIENTS In order to compute the magnitude of the desired frequency component, values of the function I,(cB.) are required over a suitable range of arguments cBj. A useful table is gven by Dwight [6] where I,(cBj) is tabulated to five significant figures for the integral values of v from 0 to 1, and cBj from 0 to 6 in the intervals of 0.1. In addition, the values of the function Lk12(cBj) are required if (20) and (21) are used. The only modified Struve function which appears to be tabulated in the literature is for v = -2, -1, and 0.