19 Elliptic IntegralsApplications

§19.34 Mutual Inductance of Coaxial Circles

The mutual inductance M of two coaxial circles of radius a and b with centers at a distance h apart is given in cgs units by

19.34.1 c2⁢M2⁢π=a⁢b⁢∫02⁢π(h2+a2+b2−2⁢a⁢b⁢cos⁡θ)−1/2⁢cos⁡θ⁢dθ=2⁢a⁢b⁢∫−11t⁢dt(1+t)⁢(1−t)⁢(a3−2⁢a⁢b⁢t)=2⁢a⁢b⁢I⁡(𝐞5),

where c is the speed of light, and in (19.29.11),

19.34.2 a3 =h2+a2+b2,
a5 =0,
b5 =1.

The method of §19.29(ii) uses (19.29.18), (19.29.16), and (19.29.15) to produce

19.34.3 2⁢a⁢b⁢I⁡(𝐞5)=a3⁢I⁡(𝟎)−I⁡(𝐞3)=a3⁢I⁡(𝟎)−r+2⁢r−2⁢I⁡(−𝐞3)=2⁢a⁢b⁢(I⁡(𝟎)−r−2⁢I⁡(𝐞1−𝐞3)),

where a1+b1⁢t=1+t and

19.34.4 r±2=a3±2⁢a⁢b=h2+(a±b)2

is the square of the maximum (upper signs) or minimum (lower signs) distance between the circles. Application of (19.29.4) and (19.29.7) with α=1, aβ+bβ⁢t=1−t, δ=3, and aγ+bγ⁢t=1 yields

19.34.5 3⁢c28⁢π⁢a⁢b⁢M=3⁢RF⁡(0,r+2,r−2)−2⁢r−2⁢RD⁡(0,r+2,r−2),

or, by (19.21.3),

19.34.6 c22⁢π⁢M=(r+2+r−2)⁢RF⁡(0,r+2,r−2)−4⁢RG⁡(0,r+2,r−2).

A simpler form of the result is

19.34.7 M=(2/c2)⁢(π⁢a2)⁢(π⁢b2)⁢R−32⁡(32,32;r+2,r−2).

References for other inductance problems solvable in terms of elliptic integrals are given in Grover (1946, pp. 8 and 283).