The potential energy of a particle of mass $m$ situated in a unidimensional potential field varies as $U(x) = U_0(1 - \cos ax)$,where $U_0$ and $a$ are constants. The time period of small oscillations of the particle about the mean position is

  • A
    $2\pi \sqrt{\frac{m}{a^2 U_0}}$
  • B
    $2\pi \sqrt{\frac{am}{U_0}}$
  • C
    $2\pi \sqrt{\frac{m}{a U_0}}$
  • D
    $2\pi \sqrt{\frac{a^2 m}{U_0}}$

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