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 ,