In above diagram, ma=pseudo force due to acceleration of plank,
$f=$ force of static friction, $m g=$ weight of block and $N=$ normal reaction.
Here, we must note that due to motion of plank, normal reaction force does not passes through centre of mass.
If line of action of normal force at a distance $x$ from centre, then for equilibrium of block, net torque about centre of mass must be zero.
$\Rightarrow \quad \tau_{\substack{\text { Normal } \\ \text { reaction }}}=\tau_{\text {Friction }}$
$m g$ and $m a$ does not produces any torque about centre of mass as their line of action passes through centre of mass.
$\Rightarrow N \cdot x=f \cdot l / 2$
$\Rightarrow m g x=m a \frac{l}{2}$
${[\because N=m g \text { and } f=m a]}$
$\Rightarrow x=\left(\frac{a}{g}\right) \frac{l}{2}$
$\text { or } x=\frac{1}{10} \cdot \frac{l}{2} \quad\left[\because a=\frac{g}{10}\right]$
$\text { or } x=\frac{l}{20}$
So, coordinates of point from which reaction passes are $\left(-\frac{l}{20}, 0\right)$.
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| Column $I$ | Column $II$ |
| $(A)$ Horizontal component of velocity | $(p)$ $5$ SI unit |
| $(B)$ Vertical component of velocity | $(q)$ $10$ SI unit |
| $(C)$ Horizontal displacement | $(r)$ $15$ SI unit |
| $(D)$ Vertical displacement | $(s)$ $20$ SI unit |
