A ball is hung vertically by a thread of length 'l' from a point of an inclined wall that makes an angle with the vertical. The thread with the ball is then deviated through a small angle α(α>β) and set free. Assuming the wall to be perfectly elastic, the period of such pendulum is
2√lg[π2+sin−1(βα)]
T=T02+2t=π√lg+2t …(i)
t→ time to travel from O to β angle ; β=α sinω t
t=1ωsin−1(βα)⇒t=T02πsin−1(βα)
Here T0=2π√lg
Putting value of t in eqn (1)
T=2√lg[π2+sin−1(βα)]