Given : T = 2π s, v = \(b\sqrt{3}\) m/s at x=b
ω = 2π/T = 2π/2π =1 rad/s
v = ω\(\sqrt{A^2-x^2}\)
∴ at x = b, \(b\sqrt{3}\) = (1)\(\sqrt{A^2-x^2}\)
∴ 3b2 = A2 – b2 , ∴ A = 2b
∴ Assuming the particle starts from the mean position, its displacement is given by
x = A sin ωt = 2b sint
If the particle is at x = b at t = t1,
b = 2b sin t1 ∴ t1= sin-1(1/2) = π/6 s
Also, with period T = 2π s, on travelling a further distance b the particle will reach the positive extremity at time t2 = π/2 s.
The time taken to travel a further distance b from x = b is t2 – t1 = π/2 − π/6 = π/3 s