Approximate Boundary Conditions in Electromagnetics

Appendix E: Determination of Constants

The constants a 1, a 2 , a 3, A 0 and A 1 in Section 5.6.2 are related by (5.213) with ? = - ? m, = ? m( m = 1, 2), and, since there are only four equations, it is clear that one constant is undetermined.

When ? = - ? 1, (5.200) becomes

(E.1)

and for ? = - ? 1 we have

(E.2)

The addition of these gives

(E.3)

where

(E.4)

and there is an equation similar to (E.3) with ? 1 replaced by ? 2. These are sufficient to specify ? 1 and ? 3 in terms of C. By expanding (sin ? m) -1 sin 3 ? m etc. in powers of cos 2 ? m and using the fact that

(E.5)

it can be shown that

(E.6)
(E.7)
(E.8)

for any ?.

To complete the specification we need another equation connecting C and ?. Subtraction of (E.2) from (E.1) gives

and there is again a similar equation with ? 1, ? 1 and ? 2 replaced by ? 2 , ? 2 and ? 1, respectively. On eliminating a 2 from the two equations, we obtain

(E.9)

where we have used the fact that

cos 3 ? m = - cos 2 ? m

and by a...

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