Right answer is (a) ∅=\(\frac{π}{2}\)
The explanation is: r= a(1-cosθ)
taking logarithms on both sides we get,
logr = loga + log(1-cosθ)
differentiating w.r.t θ we get,
\( \frac{1}{r} \frac{dr}{dθ} = 0 + \frac{sinθ}{1-cosθ}\)
\(\frac{1}{r} \frac{dr}{dθ} = \frac{2 sin \frac{θ}{2} cos\frac{θ}{2}}{2sin^2 \frac{θ}{2}} = cot\frac{θ}{2}\) ..(1),
but \(cot∅ = \frac{1}{r} \frac{dr}{dθ}\)….(2)
From (1)&(2)
∅=\(\frac{π}{2}\).