√Lg[2sin⁻¹(α/β) - π]
√Lg[π + 2sin⁻¹(α/β)]
√Lg[π - 2sin⁻¹(α/β)]
√Lg[2sin⁻¹(α/β) + π]
The motion of the string can be represented as an angular displacement from the mean position, given as:
θ = βsin(ωt)
Time taken from displacement from mean position to β and back to mean position = t₁ = T/2
where T is the time period of the oscillation without the wall barrier.
Thus t₁ = 1/2 × 2π√Lg = π√Lg
Time taken to displace from mean position to α can be found by:
α = βsin(ωt) ⇒ t = 1/ωsin⁻¹(α/β) = √Lg sin⁻¹(α/β)
Thus time taken to displace from mean position to α and back to mean position = t₂ = 2√Lg sin⁻¹(α/β)
Thus the time period of the oscillation = t₁ + t₂ = √Lg[π + 2sin⁻¹(α/β)]