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Circular Motion question

2022 · 26 Jun · Shift 1 · Q45
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  5. /2022 · 26 Jun · Shift 1 · Q45

Circular Motion question

2022 · 26 Jun · Shift 1 · Q45

JEE MainPhysicsCircular MotionMCQ+4 / −1
A ball is released from rest from point P of a smooth semi-spherical vessel as shown in figure. The ratio of the centripetal force and normal reaction on the ball at point Q is A while angular position of point Q is α\alphaα with respect to point P. Which of the following graphs represent the correct relation between A and α\alphaα when ball goes from Q to R? JEE Main 2022 (Online) 26th June Morning Shift Physics - Circular Motion Question 44 English
  1. A
    JEE Main 2022 (Online) 26th June Morning Shift Physics - Circular Motion Question 44 English Option 1
  2. B
    JEE Main 2022 (Online) 26th June Morning Shift Physics - Circular Motion Question 44 English Option 2
  3. C
    JEE Main 2022 (Online) 26th June Morning Shift Physics - Circular Motion Question 44 English Option 3
  4. D
    JEE Main 2022 (Online) 26th June Morning Shift Physics - Circular Motion Question 44 English Option 4
View written solutionFree

Correct answer: C

  1. Set up the motion

A small ball slides बिना friction on the inside of a smooth hemispherical vessel.

  • It is released from rest at point PPP.
  • At a general point QQQ, let the angular position from PPP be α\alphaα.

We need the relation between A=centripetal forcenormal reaction.A=\frac{\text{centripetal force}}{\text{normal reaction}}.A=normal reactioncentripetal force​.


  1. Speed of the ball at angle α\alphaα

Take radius of the vessel as RRR and mass of ball as mmm.

If the ball has moved through angle α\alphaα from the top point PPP, then its vertical drop is h=R(1−cos⁡α).h=R(1-\cos\alpha).h=R(1−cosα).

By energy conservation, mgR(1−cos⁡α)=12mv2mgR(1-\cos\alpha)=\frac12 mv^2mgR(1−cosα)=21​mv2 so v2=2gR(1−cos⁡α).v^2=2gR(1-\cos\alpha).v2=2gR(1−cosα).

Hence the required centripetal force is Fc=mv2R=2mg(1−cos⁡α).F_c=\frac{mv^2}{R}=2mg(1-\cos\alpha).Fc​=Rmv2​=2mg(1−cosα).


  1. Normal reaction at point QQQ

Since the ball is moving on the inside of the sphere, toward the center the radial force balance is N−mgcos⁡α=mv2R.N-mg\cos\alpha=\frac{mv^2}{R}.N−mgcosα=Rmv2​.

So, N=mv2R+mgcos⁡α.N=\frac{mv^2}{R}+mg\cos\alpha.N=Rmv2​+mgcosα.

Substitute mv2R=2mg(1−cos⁡α)\dfrac{mv^2}{R}=2mg(1-\cos\alpha)Rmv2​=2mg(1−cosα): N=2mg(1−cos⁡α)+mgcos⁡αN=2mg(1-\cos\alpha)+mg\cos\alphaN=2mg(1−cosα)+mgcosα N=mg(2−cos⁡α).N=mg(2-\cos\alpha).N=mg(2−cosα).


  1. Find the ratio AAA

Therefore, A=\frac{F_c}{N}=\frac{\dfrac{mv^2}{R}}{N}= rac{2mg(1-\cos\alpha)}{mg(2-\cos\alpha)}.

Thus, A=2(1−cos⁡α)2−cos⁡α.\boxed{A=\frac{2(1-\cos\alpha)}{2-\cos\alpha}}.A=2−cosα2(1−cosα)​​.


  1. Nature of the graph

Now examine how AAA changes with α\alphaα as the ball moves from QQQ to RRR.

Let x=cos⁡α.x=\cos\alpha.x=cosα. Then A=2(1−x)2−x.A=\frac{2(1-x)}{2-x}.A=2−x2(1−x)​.

As α\alphaα increases from 000 to π/2\pi/2π/2 (top to equator of hemisphere), cos⁡α\cos\alphacosα decreases from 111 to 000.

Important values:

  • At α=0\alpha=0α=0: A=2(1−1)2−1=0.A=\frac{2(1-1)}{2-1}=0.A=2−12(1−1)​=0.

  • At α=π/2\alpha=\pi/2α=π/2: A=2(1−0)2−0=1.A=\frac{2(1-0)}{2-0}=1.A=2−02(1−0)​=1.

Now check monotonicity: A(x)=2(1−x)2−xA(x)=\frac{2(1-x)}{2-x}A(x)=2−x2(1−x)​ Differentiate w.r.t. xxx: \frac{dA}{dx}=\frac{-2(2-x)-2(1-x)(-1)}{(2-x)^2}= rac{-4+2x+2-2x}{(2-x)^2}=-\frac{2}{(2-x)^2}<0. Since x=cos⁡αx=\cos\alphax=cosα decreases with increasing α\alphaα, AAA increases with α\alphaα.

Also, near α=0\alpha=0α=0, slope starts from zero and then rises smoothly; the curve is increasing and approaches 111 at π/2\pi/2π/2.

So the correct graph is the one that:

  • starts from (0,0)(0,0)(0,0),
  • increases monotonically,
  • reaches (π/2,1)(\pi/2,1)(π/2,1).

This corresponds to Option C.


  1. Comparison with stored answer

Stored correct answer = C.

My derived answer = C.

So they agree.

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