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Question: Define angle of repose. Prove that the coefficient of static friction is ‘tangent’ of the repose....

Define angle of repose. Prove that the coefficient of static friction is ‘tangent’ of the repose.

Explanation

Solution

Hint: - Angle of repose is the minimum angle that an inclined plane makes with the horizontal plane when a body placed on it just begins to slide down. For the second part, you need to first make the free body diagram and mark the angle of repose and forces that will be acting on the block. This includes limiting friction, fL{f_L}, Normal force NN, and the weight of the block mgmg. After equating all these forces in the form of an equation, use the formula for limiting friction and compare all the equations.

Formula used:
Limiting Friction, fL=μN{f_L} = \mu N where μ is the coefficient of friction, and NN is the normal force acting on the block.

Step-by-step solution:


Make the diagram of the block as shown. mgmg is the weight of the block acting vertically downward, NN is the normal force acting perpendicular to the diagonal surface of ramp, fL{f_L} is the limiting friction acting in the opposite direction of motion of block along the diagonal surface of the ramp, α\alpha is the angle of repose, mgcosxmg\cos x and mgsinxmg\sin x are the respective components of force mgmg.
Now, we know that angle α\alpha will be equal to the angle xx. Therefore,
mgcosxmg\cos x = mgcosαmg\cos \alpha
mgsinxmg\sin x = mgsinαmg\sin \alpha .
NN = mgcosαmg\cos \alpha (net force on a static object = 0) ------equation(1){\text{equation(1)}}
Also, fL{f_L} = mgsinαmg\sin \alpha (net force on a static object = 0)
We know that fL=μN{f_L} = \mu N
Substituting the values of NN and fL{f_L} in the above equation, we get, mgsinαmg\sin \alpha = μN\mu N
mgsinαmg\sin \alpha = μ\mu × mgcosαmg\cos \alpha (using equation(1){\text{equation(1)}})
On simplifying, we get,
sinα\sin \alpha = μ\mu × cosα\cos \alpha (mgmg gets canceled)
sinαcosα=μ\dfrac{{\sin \alpha }}{{\cos \alpha }} = \mu tanα=μ\tan \alpha = \mu
Hence Proved.

Note: Make a free body diagram of the block to make calculations and force markings easier. It is important to mark the forces in proper directions in the free body diagram to make all our calculations correct otherwise the complete solution may go wrong.