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Gravitation question

2014 · Shift 0 · Q69
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  5. /2014 · Shift 0 · Q69

Gravitation question

2014 · Shift 0 · Q69

JEE MainPhysicsGravitationMCQ+4 / −1
Four particles, each of mass MMM and equidistant from each other, move along a circle of radius RRR under the action of their mutual gravitational attraction. The speed of each particle is :
  1. A
    GMR\sqrt {{{GM} \over R}}RGM​​
  2. B
    22GMR\sqrt {2\sqrt 2 {{GM} \over R}}22​RGM​​
  3. C
    GMR(1+22)\sqrt {{{GM} \over R}\left( {1 + 2\sqrt 2 } \right)}RGM​(1+22​)​
  4. D
    12GMR(1+22){1 \over 2}\sqrt {{{GM} \over R}\left( {1 + 2\sqrt 2 } \right)}21​RGM​(1+22​)​
View written solutionFree

Correct answer: D

  1. Geometry of the configuration

Since four equal masses are equidistant from each other along a circle, they must be placed at the vertices of a square inscribed in a circle of radius RRR.

  • Distance between adjacent particles: a=2Ra = \sqrt{2}Ra=2​R because the side of an inscribed square is 2R\sqrt{2}R2​R.

  • Distance between opposite particles: d=2Rd = 2Rd=2R which is the diameter.


  1. Force on one particle due to the other three

Take one particle at a vertex of the square. The other three particles exert gravitational forces on it.

(i) Force due to each adjacent particle

For adjacent separation a=2Ra=\sqrt{2}Ra=2​R, F1=GM2a2=GM22R2F_1 = \frac{GM^2}{a^2} = \frac{GM^2}{2R^2}F1​=a2GM2​=2R2GM2​

There are two such forces, symmetric about the diagonal toward the center.

The angle between each adjacent-force direction and the diagonal is 45∘45^\circ45∘. Hence resultant of these two equal forces is: F12=2F1cos⁡45∘F_{12} = 2F_1\cos 45^\circF12​=2F1​cos45∘ F12=2⋅GM22R2⋅12F_{12} = 2\cdot \frac{GM^2}{2R^2}\cdot \frac{1}{\sqrt{2}}F12​=2⋅2R2GM2​⋅2​1​ F12=GM22R2F_{12} = \frac{GM^2}{\sqrt{2}R^2}F12​=2​R2GM2​

This resultant is directed toward the center.

(ii) Force due to the opposite particle

Opposite separation is 2R2R2R, so F2=GM2(2R)2=GM24R2F_2 = \frac{GM^2}{(2R)^2} = \frac{GM^2}{4R^2}F2​=(2R)2GM2​=4R2GM2​ This also acts along the same diagonal, toward the center.


  1. Net gravitational force toward the center

Thus total inward force on one particle is Fnet=F12+F2F_{\text{net}} = F_{12} + F_2Fnet​=F12​+F2​ Fnet=GM22R2+GM24R2F_{\text{net}} = \frac{GM^2}{\sqrt{2}R^2} + \frac{GM^2}{4R^2}Fnet​=2​R2GM2​+4R2GM2​

Write 12=22\frac{1}{\sqrt{2}} = \frac{\sqrt{2}}{2}2​1​=22​​: Fnet=GM2R2(22+14)F_{\text{net}} = \frac{GM^2}{R^2}\left(\frac{\sqrt{2}}{2} + \frac14\right)Fnet​=R2GM2​(22​​+41​) Fnet=GM2R2⋅1+224F_{\text{net}} = \frac{GM^2}{R^2}\cdot \frac{1+2\sqrt{2}}{4}Fnet​=R2GM2​⋅41+22​​


  1. Use centripetal force condition

Each particle moves in a circle of radius RRR, so required centripetal force is Mv2R\frac{Mv^2}{R}RMv2​

Hence, Mv2R=GM2R2⋅1+224\frac{Mv^2}{R} = \frac{GM^2}{R^2}\cdot \frac{1+2\sqrt{2}}{4}RMv2​=R2GM2​⋅41+22​​

Cancel MMM and one factor of RRR: v2=GMR⋅1+224v^2 = \frac{GM}{R}\cdot \frac{1+2\sqrt{2}}{4}v2=RGM​⋅41+22​​

Therefore, v=12GMR(1+22)v = \frac12\sqrt{\frac{GM}{R}(1+2\sqrt{2})}v=21​RGM​(1+22​)​


  1. Match with options

This matches: D: 12GMR(1+22)\boxed{\text{D: } \frac12\sqrt{\frac{GM}{R}(1+2\sqrt{2})}}D: 21​RGM​(1+22​)​​


  1. Comparison with stored correct answer

Stored correct answer: D

Our derived answer: D

So the derived answer agrees with the stored answer.

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