A block of mass $m$ lying on a rough horizontal plane is acted upon by a horizontal force $P$ and another force $Q$ inclined at an angle $\theta $ to the vertical. The block will remain in equilibrium, if the coefficient of friction between it and the surface is
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(a) By drawing the free body diagram of the block for critical condition

$F = \mu \,R$ $⇒$ $P + Q\sin \theta $

$ = \mu \,(mg + Q\cos \theta )$

$\therefore \mu = \frac{{P + Q\sin \theta }}{{mg + Q\cos \theta }}$

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