When a particle of mass $m$ is attached to a vertical spring of spring constant $k$ and released,its motion is described by $y(t) = y_{0} \sin^{2} \omega t$,where $y$ is measured from the lower end of the unstretched spring. Then $\omega$ is

  • A
    $\sqrt{\frac{g}{y_{0}}}$
  • B
    $\sqrt{\frac{g}{2y_{0}}}$
  • C
    $\frac{1}{2} \sqrt{\frac{g}{y_{0}}}$
  • D
    $\sqrt{\frac{2g}{y_{0}}}$

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