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Question: Two-point masses having mass \(M\) and \(4M\) are placed at a distance \(r\). The gravitational pote...

Two-point masses having mass MM and 4M4M are placed at a distance rr. The gravitational potential at a point, where gravitational field intensity zero is-
(A) 9GMr\dfrac{{ - 9GM}}{r}
(B) 2GM3r\dfrac{{ - 2GM}}{{3r}}
(C) 3GMr\dfrac{{ - 3GM}}{r}
(D) 6GM5r\dfrac{{ - 6GM}}{{5r}}

Explanation

Solution

As we all know that the gravitational field is zero where the force of gravitation applied by both the bodies on a unit mass placed in between the line of action of the force of two bodies is equal and hence the net force at a point becomes zero.

Complete answer:
Consider the gravitational field at a point PP is equal to zero which is located at a distance xx from mass MM . Assume that a unit mass is located at a point PP.

As we all know that subsequently, the gravitational field at a point PP is zero, so it can be said that the gravitational pull exerted by the body of mass MM on a unit mass at PP i.e. F1{F_1} is equal to the gravitational pull exerted by the body of mass 4M4M on a unit mass i.e. F2{F_2}.
Therefore, we can say that the relationship becomes,
F1=F2{F_1} = {F_2}
GMx2=G(4M)(rx)2\Rightarrow \dfrac{{GM}}{{{x^2}}} = \dfrac{{G\left( {4M} \right)}}{{{{\left( {r - x} \right)}^2}}}
Taking   GM\;GM both the sides common and cancelling out we get,
(rx)2x2=4\dfrac{{{{\left( {r - x} \right)}^2}}}{{{x^2}}} = 4
(rx)x=2\Rightarrow \dfrac{{\left( {r - x} \right)}}{x} = 2
On further solving the above equation we get,
x=r3x = \dfrac{r}{3}
Now we will find the Gravitational potential at the point PP. So the gravitational potential VP{V_P} at point PP is,
VP=GMxG(4M)rx{V_P} = \dfrac{{ - GM}}{x} - \dfrac{{G\left( {4M} \right)}}{{r - x}} .............. (1)\left( 1 \right)
We will substitute x=r3x = \dfrac{r}{3} in the equation (1)\left( 1 \right) and the result would become;
VP=GMr34GMrr3{V_P} = - \dfrac{{GM}}{{\dfrac{r}{3}}} - \dfrac{{4GM}}{{r - \dfrac{r}{3}}}
VP=GMr34GM2r3\Rightarrow {V_P} = - \dfrac{{GM}}{{\dfrac{r}{3}}} - \dfrac{{4GM}}{{\dfrac{{2r}}{3}}}
On further solving the above equation we get,
VP=2GM4GM2r3{V_P} = \dfrac{{ - 2GM - 4GM}}{{\dfrac{{2r}}{3}}}
VP=9GMr\Rightarrow {V_P} = - \dfrac{{9GM}}{r}
At the point where the gravitational field is zero, the gravitational potential is equal to 9GMr- \dfrac{{9GM}}{r} .

Therefore, the correct answer to this question is (A) 9GMr- \dfrac{{9GM}}{r} .

Note:
As we all know, the work done per unit mass that is required to move an object from another location to some reference fixed point, is called Gravitational potential. It is analogous to electric potential and here the mass plays the role of the charge.