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Gravitation question

2020 · 4 Sep · Shift 1 · Q45
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Gravitation question

2020 · 4 Sep · Shift 1 · Q45

JEE MainPhysicsGravitationMCQ+4 / −1
On the x-axis and at a distance x from the origin, the gravitational field due a mass distribution is given by Ax(x2+a2)3/2{{Ax} \over {{{\left( {{x^2} + {a^2}} \right)}^{3/2}}}}(x2+a2)3/2Ax​ in the x-direction. The magnitude of gravitational potential on the x-axis at a distance x, taking its value to be zero at infinity, is:
  1. A
    A(x2+a2)3/2{A{{\left( {{x^2} + {a^2}} \right)}^{3/2}}}A(x2+a2)3/2
  2. B
    A(x2+a2)1/2{A{{\left( {{x^2} + {a^2}} \right)}^{1/2}}}A(x2+a2)1/2
  3. C
    A(x2+a2)1/2{A \over {{{\left( {{x^2} + {a^2}} \right)}^{1/2}}}}(x2+a2)1/2A​
  4. D
    A(x2+a2)3/2{A \over {{{\left( {{x^2} + {a^2}} \right)}^{3/2}}}}(x2+a2)3/2A​
View written solutionFree

Correct answer: C

  1. Given gravitational field

On the x-axis, the gravitational field is

g⃗(x)=Ax(x2+a2)3/2 i^\vec g(x)=\frac{Ax}{(x^2+a^2)^{3/2}}\,\hat ig​(x)=(x2+a2)3/2Ax​i^

We need the magnitude of gravitational potential V(x)V(x)V(x), with

V(∞)=0.V(\infty)=0.V(∞)=0.
  1. Relation between field and potential

For one-dimensional motion along x,

gx=−dVdxg_x=-\frac{dV}{dx}gx​=−dxdV​

So,

−dVdx=Ax(x2+a2)3/2-\frac{dV}{dx}=\frac{Ax}{(x^2+a^2)^{3/2}}−dxdV​=(x2+a2)3/2Ax​

Hence,

dVdx=−Ax(x2+a2)3/2.\frac{dV}{dx}=-\frac{Ax}{(x^2+a^2)^{3/2}}.dxdV​=−(x2+a2)3/2Ax​.
  1. Integrate to get potential

Integrate with respect to xxx:

V(x)=∫−Ax(x2+a2)3/2 dxV(x)=\int -\frac{Ax}{(x^2+a^2)^{3/2}}\,dxV(x)=∫−(x2+a2)3/2Ax​dx

Let

u=x2+a2⇒dν=2x dxu=x^2+a^2 \quad \Rightarrow \quad d\nu=2x\,dxu=x2+a2⇒dν=2xdx

Then,

V(x)=−A∫x dx(x2+a2)3/2V(x)=-A\int \frac{x\,dx}{(x^2+a^2)^{3/2}}V(x)=−A∫(x2+a2)3/2xdx​

Using the standard result,

∫x dx(x2+a2)3/2=−1x2+a2+C\int \frac{x\,dx}{(x^2+a^2)^{3/2}}=-\frac{1}{\sqrt{x^2+a^2}}+C∫(x2+a2)3/2xdx​=−x2+a2​1​+C

Therefore,

V(x)=−A(−1x2+a2)+CV(x)= -A\left(-\frac{1}{\sqrt{x^2+a^2}}\right)+CV(x)=−A(−x2+a2​1​)+C V(x)=Ax2+a2+CV(x)=\frac{A}{\sqrt{x^2+a^2}}+CV(x)=x2+a2​A​+C
  1. Apply boundary condition

Given V(∞)=0V(\infty)=0V(∞)=0.

As x→∞x\to\inftyx→∞,

Ax2+a2→0\frac{A}{\sqrt{x^2+a^2}}\to 0x2+a2​A​→0

So,

C=0.C=0.C=0.

Thus,

V(x)=Ax2+a2.V(x)=\frac{A}{\sqrt{x^2+a^2}}.V(x)=x2+a2​A​.
  1. Magnitude of gravitational potential

The required magnitude is

Ax2+a2\boxed{\frac{A}{\sqrt{x^2+a^2}}}x2+a2​A​​
  1. Match with options

This corresponds to:

Option C

A(x2+a2)1/2\boxed{\frac{A}{(x^2+a^2)^{1/2}}}(x2+a2)1/2A​​
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