MCQMediumJEE 2023Friction (Static, Kinetic, Rolling)

JEE Physics 2023 Question with Solution

As shown in the figure, a block of mass 10kg10 \, \text{kg} lying on a horizontal surface is pulled by a force FF acting at an angle 3030^\circ with horizontal. For μs=0.25\mu_s = 0.25, the block will just start to move for the value of FF: [Given g=10m s2g = 10 \, \text{m s}^{-2}]

A block on a rough horizontal surface is pulled by a force F inclined at 30 degrees above the horizontal, with g = 10 m s^-2 indicated.
  • A

    33.3N33.3 \, \text{N}

  • B

    25.2N25.2 \, \text{N}

  • C

    20N20 \, \text{N}

  • D

    35.7N35.7 \, \text{N}

Answer

Correct answer:D

Step-by-step solution

Standard Method

Given: Mass of block is 10kg10 \, \text{kg}, coefficient of static friction is μs=0.25\mu_s = 0.25, angle of pull is 3030^\circ, and g=10m/s2g = 10 \, \text{m/s}^2.

Find: The value of FF for which the block just starts to move.

Resolve the applied force into horizontal and vertical components:

Fcos30andFsin30F \cos 30^\circ \quad \text{and} \quad F \sin 30^\circ

The upward vertical component reduces the normal reaction. Therefore,

N=MgFsin30N = Mg - F \sin 30^\circ

Substituting the given values,

N=10×10F×12=100F2N = 10 \times 10 - F \times \frac{1}{2} = 100 - \frac{F}{2}

At the point of impending motion, the horizontal component of the pull equals the maximum static friction:

Fcos30=μsNF \cos 30^\circ = \mu_s N

So,

F32=0.25(100F2)F \frac{\sqrt{3}}{2} = 0.25 \left(100 - \frac{F}{2}\right) 3F2=25F8\frac{\sqrt{3}F}{2} = 25 - \frac{F}{8}

Multiplying by 88,

43F=200F4\sqrt{3}F = 200 - F F(43+1)=200F(4\sqrt{3} + 1) = 200 F=20043+125.22NF = \frac{200}{4\sqrt{3} + 1} \approx 25.22 \, \text{N}

Therefore, the required force is approximately 25.2N25.2 \, \text{N}. The numerical working matches option B, although the solution incorrectly labels it as D.

Force Balance Explanation

Given: The block is on a horizontal rough surface and is pulled upward at 3030^\circ.

Find: The pull needed to produce impending motion.

The key idea is that friction depends on the normal reaction, and the normal reaction is not equal to mgmg here because the applied force has an upward component.

  1. Vertical balance before motion:
N+Fsin30=MgN + F \sin 30^\circ = Mg

Hence,

N=MgFsin30N = Mg - F \sin 30^\circ
  1. Limiting friction:
fmax=μsNf_{\max} = \mu_s N
  1. Horizontal balance at impending motion:
Fcos30=fmaxF \cos 30^\circ = f_{\max}

Combining these,

Fcos30=μs(MgFsin30)F \cos 30^\circ = \mu_s (Mg - F \sin 30^\circ)

Using cos30=32\cos 30^\circ = \frac{\sqrt{3}}{2} and sin30=12\sin 30^\circ = \frac{1}{2},

F32=0.25(100F2)F \frac{\sqrt{3}}{2} = 0.25\left(100 - \frac{F}{2}\right)

This gives the same result,

F25.2NF \approx 25.2 \, \text{N}

So the correct choice from the given options is B.

Common mistakes

  • Using N=mgN = mg directly is wrong because the applied force has an upward component Fsin30F \sin 30^\circ that reduces the normal reaction. First write N=mgFsin30N = mg - F \sin 30^\circ.

  • Equating the whole applied force FF to friction is incorrect. Only the horizontal component Fcos30F \cos 30^\circ opposes friction along the surface, so use Fcos30=fmaxF \cos 30^\circ = f_{\max}.

  • Using kinetic friction instead of limiting static friction is a conceptual error. Since the block is about to move, the correct condition is impending motion, so friction is fmax=μsNf_{\max} = \mu_s N.

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