A particle of mass M, is executing simple harmonic oscillations of amplitude A. The maximum energy, of this oscillating particle, is E0.
The time period, T, of this oscillating particle, and its velocity vx , when it is displaced a distance \(x(=\frac{A\sqrt{3}}{2})\) from its mean position, can be expressed, in terms of E0 , as
(1) \(T = (\frac{2\pi^2 MA^2}{E_0})^{1/2} ; \,v_x =(\frac{E_0}{2M})^{1/2}\)
(2) \(T = (\frac{\pi^2 MA^2}{E_0})^{1/2} ; \,v_x =(\frac{E_0}{2M})^{1/2}\)
(3) \(T = (\frac{2\pi^2 MA^2}{E_0})^{1/2} ; \,v_x =(\frac{2E_0}{2M})^{1/2}\)
(4) \(T = (\frac{\pi^2 MA^2}{2E_0})^{1/2} ; \,v_x =(\frac{E_0}{2M})^{1/2}\)