The displacement of a particle executing simple harmonic motion is given by
$y = A_{0} + A \sin \omega t + B \cos \omega t$
Then the amplitude of its oscillation is given by

  • A
    $A_{0} + \sqrt{A^{2} + B^{2}}$
  • B
    $\sqrt{A^{2} + B^{2}}$
  • C
    $\sqrt{A_{0}^{2} + (A + B)^{2}}$
  • D
    $A + B$

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