The force required to move a body up a rough inclined plane is double the force required to prevent the body…
- $\frac{1}{3}$
- $\frac{1}{\sqrt{2}}$
- $\frac{1}{\sqrt{3}}$
- $\frac{1}{2}$
Solution

According to the question, $ \begin{aligned} & F_{\text {up }}=2 F_{\text {down }} \\ & m g(\sin \theta+\mu \cos \theta)=2 m g(\sin \theta-\mu \cos \theta) \\ & \sin \theta+\mu \cos \theta=2 \sin \theta-2 \mu \cos \theta \\ & 3 \mu \cos \theta=\sin \theta \\ & \mu=\frac{1}{3} \tan \theta \\ & \mu=\frac{1}{3} \times \tan 60^{\circ} \\ & \Rightarrow \quad \mu=\frac{1}{3} \sqrt{3}=\frac{1}{\sqrt{3}} \\ & \end{aligned} $
Asked in: AP EAMCET 2014