MCQ
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 unstretched spring. Then $\omega$ is
- A$\sqrt{\frac{g}{y_{0}}}$
- ✓$\sqrt{\frac{g}{2 y_{0}}}$
- C$\frac{1}{2} \sqrt{\frac{g}{y_{0}}}$
- D$\sqrt{\frac{2 g}{y_{0}}}$

