The angular velocity and the amplitude of a simple pendulum are $\omega$ and $A$ respectively. At a displacement $x$ from the mean position,its kinetic energy is $T$ and potential energy is $V$. Then the ratio $\frac{V}{T}$ is
- A$\frac{x^2}{A^2 - x^2}$
- B$\frac{A^2 - x^2}{x^2}$
- C$\frac{x^2 \omega^2}{A^2 - x^2}$
- D$\frac{A^2 - x^2}{x^2 \omega^2}$
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