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Question: A body is in limiting equilibrium on a rough inclined plane at angle \[{{30}^{o}}\] with horizontal....

A body is in limiting equilibrium on a rough inclined plane at angle 30o{{30}^{o}} with horizontal. Calculate the acceleration with which the body will slide down when the inclination of the plane is changed to 60o{{60}^{o}}. (Take g=10g=10m/s2s^2)

Explanation

Solution

Draw the free body diagram to find the various forces acting on the body. Find the coefficient of friction from the limiting equilibrium condition. Utilise this in calculating the acceleration with which the body slides down.

Formula used: a=Fnetm=mgsinθμmgcosθma=\dfrac{{{F}_{n}}{{_{e}}_{t}}}{m}=\dfrac{mgsin\theta -\mu mgcos\theta }{m}
aa is the acceleration of the body
Fnet{{F}_{n}}{{_{e}}_{t}} is the net force acting on the body
mm is the mass of the body
gg is the acceleration due to gravity
θ\theta is the angle of inclination of the slope
μ\mu is the coefficient of friction

Complete step by step solution:

The forces acting on the body are:
1. Force of gravity
2. Normal force
3. Frictional force

The downward gravitational force is resolved into components, parallel and perpendicular to the surface. The normal force exerted by the incline on the object is given by NNand is perpendicular to the incline surface. It exactly balances the component of gravitational force perpendicular to the surface such that N=mgcosθN=mg\cos \theta . The frictional force experienced by the body is fμNf\le \mu N and is parallel to the incline surface. This frictional force prevents the object from sliding down the incline. In the limiting condition, it is at it’s maximum possible value.

In the first case when θ=30o\theta ={{30}^{o}}, then the body is in limiting equilibrium such that Fnet=0{{F}_{n}}{{_{e}}_{t}}=0

& mg\sin \theta =\mu mgcos\theta \\\ & \mu =tan\theta \\\ & \mu =tan{{30}^{o}}=\dfrac{1}{\sqrt{3}} \\\ \end{aligned}$$ In the second case when $$\theta=60^o$$, then the body starts to slide down the incline. The acceleration is given by, $$\begin{aligned} & a=\dfrac{{{F}_{n}}{{_{e}}_{t}}}{m}=\dfrac{mgsin\theta -\mu mgcos\theta }{m} \\\ & a=g\sin {{60}^{o}}-\mu gcos{{60}^{o}}=\dfrac{10}{\sqrt{3}} m/s^2\\\ \end{aligned}$$ The body will slide down with acceleration $$a=\dfrac{10}{\sqrt{3}}$$m/$s^2$ when the inclination of the plane is increased. **Note:** The frictional force and normal force are contact forces whereas the gravitational force is non-contact force.