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The angular velocity and the amplitude of a simple pendulum is $'\omega '$ and $'A'$ respectively. At a displacement $x$ from the mean position its kinetic energy is $'T'$ and potnetial energy is $'V'$. Then the ratio $\frac{V}{T}$ is
  • A$\frac{{{x^2}{\omega ^2}}}{{{A^2} - {x^2}}}$
  • B$\frac{{{A^2} - {x^2}}}{{{x^2}{\omega ^2}}}$
  • C$\frac{{{x^2}}}{{{A^2} - {x^2}}}$
  • D$\frac{{{A^2} - {x^2}}}{{{x^2}}}$
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