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Question: Three identical bodies of equal mass \(M\) each are moving along a circle of radius R under the acti...

Three identical bodies of equal mass MM each are moving along a circle of radius R under the action of their mutual gravitational attraction. The speed of each body is: -
A) GMR\sqrt {\dfrac{{GM}}{R}}
B) GM3R\sqrt {\dfrac{{GM}}{{3R}}}
C) GM3R\sqrt {\dfrac{{GM}}{{\sqrt 3 R}}}
D) GM2R\sqrt {\dfrac{{GM}}{{\sqrt 2 R}}}

Explanation

Solution

Here each particle experiences a force of attraction from the other two bodies. Find the direction of the resultant force on a body due to the presence of other two bodies. Also calculate the value of this resultant force. As the three bodies are moving in a circle, the force of attraction on each particle must be directed towards the center of the circle.

Complete step-by-step solution: In this problem, we are given three bodies which are moving in a circle. As a result, we can say that the bodies are placed on the sides of an equilateral triangle. And the circle is known as circumcircle. We know that for a triangle with a circumcircle, the centroid and the circumcenter coincide. Let us represent it diagrammatically.

Here, the three bodies are having equal masses, GG is the centroid, aa is the length of the side of the equilateral triangle, RR is the radius of the circle.
From trigonometry, we have
a=3Ra = \sqrt 3 R --equation 11
As the bodies are identical and we have achieved that the distances between two bodies must be equal therefore, the forces acting on the three bodies must also be equal.
Let us consider the forces acting on the body at point 11 , the resultant force on this body will be towards the centre. The magnitude of this force F1{F_1} due bodies at point 22 and 33 will be

F1=F2+F3{F_1} = {F_2} + {F_3}

Force at point one due body at point two is

F1,2=GM2a2 \Rightarrow {F_{1,2}} = \dfrac{{G{M^2}}}{{{a^2}}}

Force at point one due body at point three is

F1,3=GM2a2 \Rightarrow {F_{1,3}} = \dfrac{{G{M^2}}}{{{a^2}}}

Resultant force is given by

F=F1,2+F1,3+F1,2F1,3cos60F = \sqrt {\left| {{F_{1,2}}} \right| + \left| {{F_{1,3}}} \right| + \left| {{F_{1,2}}} \right|\left| {{F_{1,3}}} \right|\cos {{60}^ \circ }}

Since the triangle is equilateral hence the angle is 60{60^ \circ }

F=GM2a2+GM2a2+2GM2a2×GM2a2×12\Rightarrow F = \sqrt {\dfrac{{G{M^2}}}{{{a^2}}} + \dfrac{{G{M^2}}}{{{a^2}}} + 2\dfrac{{G{M^2}}}{{{a^2}}} \times \dfrac{{G{M^2}}}{{{a^2}}} \times \dfrac{1}{2}}
F=3GM2a2\Rightarrow F = \sqrt {3\dfrac{{G{M^2}}}{{{a^2}}}}
F=3GM2a2\Rightarrow F = \sqrt 3 \dfrac{{G{M^2}}}{{{a^2}}}

Since the particle is moving in a circle, hence centripetal force is also acting on it and the centripetal force must be equal to the magnitude of the force acting on each body.

Mv2R=3GM2a2 \Rightarrow \dfrac{{M{v^2}}}{R} = \sqrt 3 \dfrac{{G{M^2}}}{{{a^2}}}

Here vv is the speed of the body.

Substituting a=3Ra = \sqrt 3 R from equation 11 , we get

Mv2R=3GM23R2 \Rightarrow \dfrac{{M{v^2}}}{R} = \sqrt 3 \dfrac{{G{M^2}}}{{3{R^2}}}
v=GM3R\Rightarrow v = \sqrt {\dfrac{{GM}}{{\sqrt 3 R}}}

This is the speed of each body.

Thus, option C is the correct option.

Note: The bodies were identical therefore the forces acting on the three bodies were also equal. Remember that for a triangle with circumcircle, the centroid and the circumcentre coincide. Don’t forget to account for the centripetal force and remember that the centripetal force must be balanced with the forces acting by other bodies.