$A$ point mass oscillates along the $X$-axis according to the law $x=x_0 \cos \left(\omega t-\frac{\pi}{4}\right)$. If the acceleration of the particle is written as $a=A \cos (\omega t-\delta)$, then

  • A
    $A=x_0 \omega^2, \delta=-\frac{3 \pi}{4}$
  • B
    $A=x_0, \delta=-\frac{\pi}{4}$
  • C
    $A=x_0 \omega^2, \delta=\frac{\pi}{4}$
  • D
    $A=x_0 \omega^2, \delta=\frac{3 \pi}{4}$

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Values of the acceleration $A$ of a particle moving in simple harmonic motion as a function of its displacement $x$ are given in the table below:
$A \ (mm \ s^{-2})$$16$$8$$0$$-8$$-16$
$x \ (mm)$$-4$$-2$$0$$2$$4$

The period of the motion is:

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