R′ = a e(θ + 2π)cot α ,
r = λa eθ cot α = a e(θ − β)cot α ,
and
r′ = λa e(θ + 2π)cot α = a e(θ + 2π − β)cot α .
Now in the three cases (a, b, c) represented in Fig. [278], it is plain that r′
R, respectively. That is to say,
λa e(θ + 2π)cot α
a eθ cot α ,