The bob of a simple pendulum of length $L$ is released from a position of small angular displacement $\theta$. Its linear displacement at time $t$ is ($g =$ acceleration due to gravity).

  • A
    $L \theta \cos \left[\sqrt{\frac{g}{L}} \cdot t\right]$
  • B
    $L \theta \sin \left[2 \pi \sqrt{\frac{g}{L}} \cdot t\right]$
  • C
    $L \theta \cos \left[2 \pi \sqrt{\frac{g}{L}} \cdot t\right]$
  • D
    $L \theta \sin \left[\sqrt{\frac{g}{L}} \cdot t\right]$

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