The angular velocity and the amplitude of a simple pendulum is $\mathrm{\omega }$  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

  ${\mathrm{X}}^2{\mathrm{\omega }}^2/({\mathrm{a}}^2-{\mathrm{X}}^2{\mathrm{\omega }}^2)$

• B

  ${\mathrm{X}}^2/({\mathrm{a}}^2-{\mathrm{X}}^2)$

• C

  $({\mathrm{a}}^2-{\mathrm{X}}^2{\mathrm{\omega }}^2)/{\mathrm{X}}^2{\mathrm{\omega }}^2$

• D

  $({\mathrm{a}}^2-{\mathrm{X}}^2)/{\mathrm{X}}^2$