$4\, kg$ का कोई गुटका एक क्षैतिज समतल पर रखा है (चित्र)। समतल को धीरे-धीरे तब तक आनत किया जाता है जब तक क्षेतिज से किसी कोण $\theta=15^{\circ}$ पर वह गुटका सरकना आरंभ नहीं कर देता । पृष्ठ और गुटके के बीच स्थेतिक घर्षण गुणांक क्या है ?

Answer The forces acting on a block of mass $m$ at rest on an inclined plane are $(i)$ the weight mg acting vertically downwards $(ii)$ the normal force $N$ of the plane on the block, and $(iii)$ the static frictional force $f_{ s }$ opposing the impending motion. In equilibrium, the resultant of these forces must be zero. Resolving the weight $m g$ along the two directions shown, we have

$m g \sin \theta=f_{s}, \quad m g \cos \theta=N$

As $\theta$ increases, the self-adjusting frictional force

$f_{ s }$ increases until at $\theta=\theta_{\max ^{\prime}} f_{ s }$ achieves its

maximum value, $\left(f_{s}\right)_{\max }=\mu_{s} N$

Therefore.

$\tan \theta_{\max }=\mu_{s}$ or $\theta_{\max }=\tan ^{-1} \mu_{s}$

When $\theta$ becomes Just a little more than $\theta_{\max }$. there is a small net force on the block and it begins to slide. Note that $\theta_{\max }$ depends only on

$\mu_{ s }$ and $1 s$ independent of the mass of the block.

For $\quad \theta_{\max }=15^{\circ}$

$\mu_{s}=\tan 15^{\circ}$

$=0.27$