Show that simple harmonic motion may be regarded as the projection of uniform circular motion along a diameter of the circle.

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(N/A) Consider a particle moving in a circle of radius $R$ with a constant angular speed $\omega$ in a horizontal plane.
The position of the particle at any time $t$ can be represented by the angle $\theta = \omega t$ with respect to a reference diameter.
If we project the position of the particle onto a diameter of the circle,the displacement $y$ of the projection from the center of the circle at time $t$ is given by $y = R \sin(\omega t)$.
This equation $y = R \sin(\omega t)$ represents the displacement of a particle executing simple harmonic motion $(SHM)$.
As shown in the figure,as the particle moves along the circular path through points $A, B, C, D, E, F, G$,its projection on the vertical diameter moves back and forth between the extreme points $S$ and $Q$ through the center $O$. This oscillatory motion of the projection is simple harmonic motion.

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Which of the following functions of time represent $(a)$ simple harmonic,$(b)$ periodic but not simple harmonic,and $(c)$ non-periodic motion? Give period for each case of periodic motion ($\omega$ is any positive constant):
$(a)$ $\sin \omega t - \cos \omega t$
$(b)$ $\sin^3 \omega t$
$(c)$ $3 \cos (\pi/4 - 2 \omega t)$
$(d)$ $\cos \omega t + \cos 3 \omega t + \cos 5 \omega t$
$(e)$ $\exp(-\omega^2 t^2)$
$(f)$ $1 + \omega t + \omega^2 t^2$

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