$A$ point mass oscillates along the $x$-axis according to the law $x=x_0 \cos(\omega t - \frac{\pi}{4})$. 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
    $A=x_0 \omega^2, \delta = -\frac{\pi}{4}$

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