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The upper half of an inclined plane of inclination θ\theta is perfectly smooth while the lower half is rough. A block starting from rest at the top of the plane will again come to rest at the bottom if the coefficient of friction between the block and lower half of the plane is given by:

A

μ=1tanθ\mu = \frac{1}{\tan\theta}

B

μ=2tanθ\mu = \frac{2}{\tan\theta}

C

μ=2tanθ\mu = 2\tan\theta

D

μ=tanθ\mu = \tan\theta

Step-by-Step Solution

  1. Concept (Work-Energy Theorem): The work-energy theorem states that the change in kinetic energy of a body is equal to the net work done by all the forces acting on it [NCERT Class 11, Physics Part I, Sec 5.5].
  2. Analysis:
  • The block starts from rest and comes to rest at the bottom, so the change in kinetic energy ΔK=KfKi=0\Delta K = K_f - K_i = 0.
  • Let the total length of the inclined plane be LL. The upper half (L/2L/2) is smooth, and the lower half (L/2L/2) is rough.
  • Forces doing work: Gravity acts over the entire length LL. Friction acts only over the lower half L/2L/2.
  1. Work Done Calculation:
  • Work done by gravity (WgW_g): Force is mgsinθmg\sin\theta downwards along the plane. Displacement is LL. Wg=mgLsinθW_g = mg L \sin\theta
  • Work done by friction (WfW_f): Frictional force f=μN=μmgcosθf = \mu N = \mu mg \cos\theta acts upwards along the plane (opposing motion). Displacement is L/2L/2. Wf=f×L2=(μmgcosθ)L2W_f = -f \times \frac{L}{2} = -(\mu mg \cos\theta) \frac{L}{2}
  1. Equation: Wnet=Wg+Wf=0W_{net} = W_g + W_f = 0 mgLsinθμmgLcosθ2=0mg L \sin\theta - \frac{\mu mg L \cos\theta}{2} = 0 mgLsinθ=μmgLcosθ2mg L \sin\theta = \frac{\mu mg L \cos\theta}{2} Dividing both sides by mgLcosθmgL \cos\theta: sinθcosθ=μ2\frac{\sin\theta}{\cos\theta} = \frac{\mu}{2} tanθ=μ2    μ=2tanθ\tan\theta = \frac{\mu}{2} \implies \mu = 2\tan\theta
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