An oscillating pendulum suspended from the roof of a lift which is at rest has time period $T_1$. When the lift moves up with acceleration $a$, its time period is $T_2$. When the lift moves down with acceleration $a$, its time period is $T_3$. The relation between $T_1$, $T_2$, and $T_3$ is:

  • A
    $T_1 = \frac{2T_2T_3}{\sqrt{T_2^2 + T_3^2}}$
  • B
    $T_1 = \frac{\sqrt{2}T_2T_3}{\sqrt{T_2^2 + T_3^2}}$
  • C
    $T_1 = \frac{2T_2^2 T_3^2}{\sqrt{T_2 + T_3}}$
  • D
    $T_1 = \frac{\sqrt{2}T_2^2 T_3^2}{\sqrt{T_2 + T_3}}$

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