NEET2025Physics-Solving problems in Mechanics

NEET 2025 Physics Friction MCQ Question

Type: MCQ-conceptual-Medium-Class 11

There are two inclined surfaces of equal length (L) and same angle of inclination 45° with the horizontal. One of them is rough and the other is perfectly smooth. A given body takes 2 times as much time to slide down on rough surface than on the smooth surface. The coefficient of kinetic friction (μₖ) between the object and the rough surface is close to

A

0.25

B

0.40

C

0.5

D

0.75

Correct Answer

Option D

Detailed Explanation

To solve the problem, we need to analyze the motion of a body sliding down two inclined surfaces: one smooth and one rough, both inclined at an angle of 4545^\circ with the horizontal. The key points of this problem involve calculating the time taken for the body to slide down both surfaces and using the relationship between these times to find the coefficient of kinetic friction (μk\mu_k) on the rough surface.

Motion on the Smooth Surface

  1. For the smooth incline:
    • The only force acting along the incline is the component of gravitational force, given by: F=mgsin(45)F = mg \sin(45^\circ)
    • The acceleration (asa_s) of the body down the incline is: as=gsin(45)=g12a_s = g \sin(45^\circ) = g \cdot \frac{1}{\sqrt{2}}
    • The time taken (t1t_1) to slide down the length LL can be derived from the equation of motion: L=12ast12L = \frac{1}{2} a_s t_1^2 Substituting for asa_s: L=12(g12)t12L = \frac{1}{2} \left(g \cdot \frac{1}{\sqrt{2}}\right)t_1^2 Rearranging gives: t12=2L2gt_1^2 = \frac{2L \sqrt{2}}{g} Hence, t1=2L2gt_1 = \sqrt{\frac{2L \sqrt{2}}{g}}

Motion on the Rough Surface

  1. For the rough incline:
    • Here, kinetic friction opposes the motion. The frictional force is: Ffriction=μkmgcos(45)=μkmg12F_{\text{friction}} = \mu_k mg \cos(45^\circ) = \mu_k mg \cdot \frac{1}{\sqrt{2}}
    • The net force acting down the incline is: Fnet=mgsin(45)Ffriction=mg12μkmg12F_{\text{net}} = mg \sin(45^\circ) - F_{\text{friction}} = mg \cdot \frac{1}{\sqrt{2}} - \mu_k mg \cdot \frac{1}{\sqrt{2}}
    • Thus, the acceleration (ara_r) is: ar=gsin(45)μkgcos(45)=g(12μk12)a_r = g \sin(45^\circ) - \mu_k g \cos(45^\circ) = g \left(\frac{1}{\sqrt{2}} - \mu_k \cdot \frac{1}{\sqrt{2}}\right) Simplifying gives: ar=g1μk2a_r = g \cdot \frac{1 - \mu_k}{\sqrt{2}}
    • The time taken (t2t_2) to slide down the rough incline is given by: L=12art22L = \frac{1}{2} a_r t_2^2 Substituting for ara_r: L=12(g1μk2)t22L = \frac{1}{2} \left(g \cdot \frac{1 - \mu_k}{\sqrt{2}}\right)t_2^2 Rearranging gives: t22=2L2g(1μk)t_2^2 = \frac{2L\sqrt{2}}{g(1 - \mu_k)} Hence, t2=2L2g(1μk)t_2 = \sqrt{\frac{2L\sqrt{2}}{g(1 - \mu_k)}}

Relationship Between Times

  1. Given Condition:
    • We know from the problem statement that t2=2t1t_2 = 2t_1. Squaring both sides gives: t22=4t12t_2^2 = 4t_1^2
    • Substituting the expressions for t12t_1^2 and t22t_2^2: 2L2g(1μk)=42L2g\frac{2L\sqrt{2}}{g(1 - \mu_k)} = 4 \cdot \frac{2L\sqrt{2}}{g}
    • Simplifying, we can cancel out LL and 2\sqrt{2}: 11μk=4\frac{1}{1 - \mu_k} = 4
    • Rearranging gives: 1μk=141 - \mu_k = \frac{1}{4} μk=114=34\mu_k = 1 - \frac{1}{4} = \frac{3}{4}

Thus, the coefficient of kinetic friction (μk\mu_k) is:

μk=0.75\mu_k = 0.75

Conclusion

The correct answer is D) 0.75.

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