JEE Challenger
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Normal Reaction Acting on Block at Point Q

Comprehension Passage

A small block of mass 1 kg1\text{ kg} is released from rest at the top of a rough track. The track is a circular arc of radius 40 m40\text{ m}. The block slides along the track without toppling and a frictional force acts on it in the direction opposite to the instantaneous velocity. The work done in overcoming the friction up to the point QQ, as shown in the figure below, is 150 J150\text{ J}. (Take the acceleration due to gravity, g=10 m s−2g = 10\text{ m s}^{-2}).

Passage Diagram 1

Calculate the magnitude of the normal force exerted on the block at point QQ.

Options

A

7.5 N7.5\text{ N}

Correct
B

8.6 N8.6\text{ N}

C

11.5 N11.5\text{ N}

D

22.5 N22.5\text{ N}

Step-by-Step Solution

To find the magnitude of the normal force exerted on the block at point QQ, we analyze the geometry of the track and apply the principles of circular motion and the Work-Energy Theorem.

Step 1: Geometry of the Track and Position of Point QQ

The circular track has a radius R=40 mR = 40\text{ m} with its center located at P(R,R)P(R, R).

  • At the top of the track, the block starts from rest at height yi=Ry_i = R.

  • Point QQ lies on the circular arc such that the radius vector PQPQ makes an angle of 30∘30^\circ below the horizontal line PRPR.

  • The vertical coordinate of point QQ is given by: yQ=R−Rsin⁡30∘y_Q = R - R \sin 30^\circ

  • Thus, the vertical distance fallen by the block from the top to point QQ is: h=yi−yQ=Rsin⁡30∘=40×sin⁡30∘=20 mh = y_i - y_Q = R \sin 30^\circ = 40 \times \sin 30^\circ = 20\text{ m}


Step 2: Determination of Speed at Point QQ

By the Work-Energy Theorem, the total work done on the block as it moves from the top to point QQ equals the change in its kinetic energy:

Wgravity+Wfriction=12mv2−0W_{\text{gravity}} + W_{\text{friction}} = \frac{1}{2} m v^2 - 0

Given:

  • Mass m=1 kgm = 1\text{ kg}
  • g=10 m s−2g = 10\text{ m s}^{-2}
  • Wgravity=mgh=(1)(10)(20)=200 JW_{\text{gravity}} = mgh = (1)(10)(20) = 200\text{ J}
  • Work done against friction is 150 J150\text{ J}, so Wfriction=−150 JW_{\text{friction}} = -150\text{ J}

Substituting these values into the equation: 200−150=12(1)v2200 - 150 = \frac{1}{2}(1)v^2 50=12v2  ⟹  v2=100 m2s−250 = \frac{1}{2}v^2 \implies v^2 = 100\text{ m}^2\text{s}^{-2}


Step 3: Calculation of Normal Force at Point QQ

At point QQ, the forces acting on the block along the radial direction (towards the center PP) are:

  1. The normal force NN directed radially inwards towards PP.
  2. The radial component of gravity pointing radially outwards away from PP, given by mgsin⁡30∘mg \sin 30^\circ.

The net force directed towards the center provides the required centripetal force for circular motion:

N−mgsin⁡30∘=mv2RN - mg \sin 30^\circ = \frac{m v^2}{R}

Rearranging to solve for NN:

N=mgsin⁡30∘+mv2RN = mg \sin 30^\circ + \frac{m v^2}{R}

Substituting the known values:

N=(1)(10)(12)+(1)(100)40N = (1)(10)\left(\frac{1}{2}\right) + \frac{(1)(100)}{40} N=5+2.5=7.5 NN = 5 + 2.5 = 7.5\text{ N}

Thus, the magnitude of the normal force exerted on the block at point QQ is 7.5 N7.5\text{ N}.