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The angular velocity and the amplitude of a simple pendulum is  and a respectively. At a displacement X from the mean position if its kinetic energy is T and potential energy is V, then the ratio of T to V is

(a)     ${X}^{2}{\omega }^{2}\left({a}^{2}-{X}^{2}{\omega }^{2}\right)$        (b)    ${X}^{2}/\left({a}^{2}-{x}^{2}\right)$

(c)   $\left({a}^{2}-{X}^{2}{\omega }^{2}\right)/{X}^{2}{\omega }^{2}$        (d)   $\left({a}^{2}-{x}^{2}\right)/{X}^{2}$