Where $k,k_0,k_1$ and $a$ are all positive
$a=-\frac{d^{2} x}{d t^{2}}=-w^{2} x$
$w=\sqrt{\frac{k}{m}}$
$-wherein$
$x=A \sin (w t+\delta)$
$a=-K x$
$ x =x+a$
where $ a=-K(x+a)$
In $ S.H.M $ acceleration is directly proportional to the displacement from the mean position
Also the acceleration is in the opposite direction of displacement
| Column $I$ | Column $II$ |
| $(A)$ Potential energy of a simple pendulum (y axis) as a function of displacement ( $\mathrm{x}$ axis) | $Image$ |
| $(B)$ Displacement (y axis) as a function of time (x axis) for a one dimensional motion at zero or constant acceleration when the body is moving along the positive $\mathrm{x}$-direction | $Image$ |
| $(C)$ Range of a projectile (y axis) as a function of its velocity ( $\mathrm{x}$ axis) when projected at a fixed angle | $Image$ |
| $(D)$ The square of the time period (y axis) of a simple pendulum as a function of its length ( $\mathrm{x}$ axis) | $Image$ |
