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Show that for a particle executing SHM, velocity and displacement have a phase difference of \frac{\pi}{2}.

Answers (1)

Let us consider x = A \sin \omega t to be a SHM          …….. (i)

Now, v = \frac{dx}{dt}

           = A\omega \cos \omega t

            = A\omega \sin (90^{\circ} + \omega t)        …….. [since \sin (90^{\circ} + \theta ) = \cos \theta]

 Thus, v = A\omega \sin \left (\omega t + \left ( \frac{\pi}{2} \right ) \right )

From (i), we know that,

The phase of displacement  = \omega t

& from (ii), we know that,

The phase of velocity = \left (\omega t + \left ( \frac{\pi}{2} \right ) \right )

Thus, the phase difference = \omega t + \frac{\pi}{2} - \omega t

                                                = \frac{\pi}{2}.
 

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