About the Project
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 c2M2π=ab02π(h2+a2+b22abcosθ)1/2cosθdθ=2ab11tdt(1+t)(1t)(a32abt)=2abI(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 2abI(𝐞5)=a3I(𝟎)I(𝐞3)=a3I(𝟎)r+2r2I(𝐞3)=2ab(I(𝟎)r2I(𝐞1𝐞3)),

where a1+b1t=1+t and

19.34.4 r±2=a3±2ab=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+bβt=1t, δ=3, and aγ+bγt=1 yields

19.34.5 3c28πabM=3RF(0,r+2,r2)2r2RD(0,r+2,r2),

or, by (19.21.3),

19.34.6 c22πM=(r+2+r2)RF(0,r+2,r2)4RG(0,r+2,r2).

A simpler form of the result is

19.34.7 M=(2/c2)(πa2)(πb2)R32(32,32;r+2,r2).

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

pFad - Phonifier reborn

Pfad - The Proxy pFad of © 2024 Garber Painting. All rights reserved.

Note: This service is not intended for secure transactions such as banking, social media, email, or purchasing. Use at your own risk. We assume no liability whatsoever for broken pages.


Alternative Proxies:

Alternative Proxy

pFad Proxy

pFad v3 Proxy

pFad v4 Proxy