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Question: A small block starts slipping down from a point B on an inclined plane AB, which is making an angle ...

A small block starts slipping down from a point B on an inclined plane AB, which is making an angle θ\theta with the horizontal section, BC is smooth and the remaining section CA is rough with a coefficient of friction μ\mu. It is found that the block comes to rest as it reaches the bottom (point A) of the inclined plane. If BC = 2AC, the coefficient of friction is given by m = k tanθ\theta. The value of k is _______.

Answer

3

Explanation

Solution

The problem can be solved using the Work-Energy Theorem, which states that the net work done on an object is equal to the change in its kinetic energy (Wnet=ΔKEW_{net} = \Delta KE).

1. Identify Initial and Final States:

  • Initial state: Block at point B, starts slipping, so initial velocity vB=0v_B = 0.
  • Final state: Block at point A, comes to rest, so final velocity vA=0v_A = 0.
  • Therefore, the change in kinetic energy ΔKE=KEAKEB=12mvA212mvB2=00=0\Delta KE = KE_A - KE_B = \frac{1}{2}mv_A^2 - \frac{1}{2}mv_B^2 = 0 - 0 = 0.

2. Calculate Work Done by Forces: The forces doing work on the block are gravity and friction.

  • Work done by gravity (WgW_g): The block moves from B to A. The vertical height descended is hBAh_{BA}. Let the length of section AC be LL. Given BC=2ACBC = 2AC, so BC=2LBC = 2L. The total length of the inclined plane is AB=AC+BC=L+2L=3LAB = AC + BC = L + 2L = 3L. The vertical height descended is hBA=ABsinθ=(3L)sinθh_{BA} = AB \sin\theta = (3L) \sin\theta. Work done by gravity is Wg=mghBA=mg(3Lsinθ)W_g = mg h_{BA} = mg (3L \sin\theta).

  • Work done by friction (WfW_f): Friction acts only on the rough section CA. The length of this section is LL. The normal force on the inclined plane is N=mgcosθN = mg \cos\theta. The force of kinetic friction is fk=μN=μmgcosθf_k = \mu N = \mu mg \cos\theta. Since friction opposes motion, the work done by friction is negative. Wf=fk×(distance CA)=(μmgcosθ)LW_f = -f_k \times (\text{distance CA}) = -(\mu mg \cos\theta) L.

3. Apply Work-Energy Theorem: Wnet=Wg+Wf=ΔKEW_{net} = W_g + W_f = \Delta KE Since ΔKE=0\Delta KE = 0: mg(3Lsinθ)μmgLcosθ=0mg (3L \sin\theta) - \mu mg L \cos\theta = 0

4. Solve for μ\mu: Divide the entire equation by mgLmgL (assuming m,g,Lm, g, L are non-zero): 3sinθμcosθ=03 \sin\theta - \mu \cos\theta = 0 μcosθ=3sinθ\mu \cos\theta = 3 \sin\theta μ=3sinθcosθ\mu = 3 \frac{\sin\theta}{\cos\theta} μ=3tanθ\mu = 3 \tan\theta

5. Determine the value of k: The problem states that the coefficient of friction is given by μ=ktanθ\mu = k \tan\theta. Comparing our derived expression for μ\mu with the given form: 3tanθ=ktanθ3 \tan\theta = k \tan\theta Therefore, k=3k = 3.

The final answer is 3\boxed{3}.