Question:

Four identical particles of equal masses $1 kg$ made to move along the circumference of a circle of radius $1 m$ under the action of their own mutual gravitational attraction. The speed of each particle will be :

Updated On: Sep 14, 2024
  • $\sqrt{\frac{ G }{2}(1+2 \sqrt{2})}$
  • $\sqrt{ G (1+2 \sqrt{2})}$
  • $\sqrt{\frac{ G }{2}(2 \sqrt{2}-1)}$
  • $\sqrt{\frac{(1+2 \sqrt{2}) G }{2}}$
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The Correct Option is D

Solution and Explanation

$F _{1}=\frac{ Gmm }{(2 R )^{2}}=\frac{ Gm ^{2}}{4 R ^{2}}$
$F _{2}=\frac{ Gmm }{(\sqrt{2} R )^{2}}=\frac{ Gm ^{2}}{2 R ^{2}}$
$F _{3}=\frac{ Gmm }{(\sqrt{2} R )^{2}}=\frac{ Gm ^{2}}{2 R ^{2}}$
$\Rightarrow F _{ net }= F _{1}+ F _{2} \cos 45^{\circ}+ F _{3} \cos 45^{\circ}$
$=\frac{ Gm ^{2}}{4 R ^{2}}+\frac{ Gm ^{2}}{2 R ^{2}} \frac{1}{\sqrt{2}}+\frac{ Gm ^{2}}{2 R ^{2}} \frac{1}{\sqrt{2}}$
$=\frac{ Gm ^{2}}{ R ^{2}}\left(\frac{1}{4}+\frac{1}{2 \sqrt{2}}+\frac{1}{2 \sqrt{2}}\right)$
$=\frac{ Gm ^{2}}{ R ^{2}}\left(\frac{1}{4}+\frac{1}{\sqrt{2}}\right)=\frac{ Gm ^{2}}{4 R ^{2}}(1+2 \sqrt{2})$
$F _{ net }=\frac{ Gm ^{2}}{4 R ^{2}}(1+2 \sqrt{2})=\frac{ mv ^{2}}{ R }$
$\Rightarrow v =\frac{\sqrt{ G (1+2 \sqrt{2})}}{2}$
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Concepts Used:

Newtons Law of Gravitation

Gravitational Force

Gravitational force is a central force that depends only on the position of the test mass from the source mass and always acts along the line joining the centers of the two masses.

Newton’s Law of Gravitation:

According to Newton’s law of gravitation, “Every particle in the universe attracts every other particle with a force whose magnitude is,

  • Directly proportional to the product of their masses i.e. F ∝ (M1M2) . . . . (1)
  • Inversely proportional to the square of the distance between their center i.e. (F ∝ 1/r2) . . . . (2)

By combining equations (1) and (2) we get,

F ∝ M1M2/r2

F = G × [M1M2]/r2 . . . . (7)

Or, f(r) = GM1M2/r2 [f(r)is a variable, Non-contact, and conservative force]