$A$ point mass oscillates along the $x$-axis according to $x = x_0 \sin \left(\omega t - \frac{\pi}{6}\right)$. If the acceleration of the point mass is written as $a = A \sin (\omega t + \delta)$,then:

  • A
    $A = x_0, \delta = -\frac{\pi}{6}$
  • B
    $A = x_0 \omega^2, \delta = -\frac{\pi}{6}$
  • C
    $A = x_0 \omega^2, \delta = \frac{\pi}{6}$
  • D
    $A = x_0 \omega^2, \delta = \frac{5\pi}{6}$

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