(b) For rotational equilibrium about point “$P$”,
$mg\sin\theta\left( \frac{b}{2} \right) = mg\cos\theta\left( \frac{a}{2} \right)$
[image:5_image287.emf]
$\Rightarrow \tan\theta = \frac{a}{b} = \frac{10}{15} = \frac{2}{3}$
$\Rightarrow \ \theta = 33.69{^\circ}$
$i.e$., toppling starts at $\theta = 33.69{^\circ}$
and angle of repose $= \tan^{- 1}{(\mu)} = \tan^{- 1}{(\sqrt{3}}) = 60{^\circ}$
It mean the block will remain at rest on the plane up to certain angle $\theta$ and then it will topple