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Question

A solid sphere of constant density p has mass M and radius R. What is the gravitational potential difference between a point P which is at distance \(\frac{R}{2}\) from the central and its surface?

(i.e. Vp - Vsurface)

The correct answer is \(\rm -\frac{3GM}{8R}\)

Understanding Gravitational Potential Difference

The question asks us to find the gravitational potential difference between a point P located at a distance \(\frac{R}{2}\) from the center of a solid sphere and a point on its surface. The solid sphere has constant density \(\rho\), mass M, and radius R. Calculating the gravitational potential difference requires knowing the gravitational potential at both points.

Gravitational Potential Inside a Solid Sphere

For a solid sphere of uniform density, the gravitational potential at a distance \(r\) from the center, where \(r < R\), is given by the formula: $$V(r) = -\frac{GM}{2R^3}(3R^2 - r^2)$$ Here, \(G\) is the gravitational constant, M is the total mass of the solid sphere, and R is its radius. This formula describes the gravitational potential inside the solid sphere.

Gravitational Potential on the Surface of a Solid Sphere

The gravitational potential on the surface of a solid sphere (at \(r = R\)) is given by the standard formula for the potential outside a sphere (or on its surface), considering the mass is concentrated at the center for \(r \ge R\): $$V(R) = -\frac{GM}{R}$$ This gives the gravitational potential at the outer boundary of the solid sphere.

Calculating Potential at Point P (\(r = \frac{R}{2}\))

Point P is located at a distance \(r = \frac{R}{2}\) from the center, which is inside the solid sphere (\(\frac{R}{2} < R\)). We use the formula for the potential inside the solid sphere: $$V_P = V\left(\frac{R}{2}\right) = -\frac{GM}{2R^3}\left(3R^2 - \left(\frac{R}{2}\right)^2\right)$$ Now, let's simplify the expression: $$V_P = -\frac{GM}{2R^3}\left(3R^2 - \frac{R^2}{4}\right)$$ $$V_P = -\frac{GM}{2R^3}\left(\frac{12R^2 - R^2}{4}\right)$$ $$V_P = -\frac{GM}{2R^3}\left(\frac{11R^2}{4}\right)$$ $$V_P = -\frac{11GM}{8R}$$ So, the gravitational potential at point P is \(-\frac{11GM}{8R}\).

Calculating Potential at the Surface (\(r = R\))

The potential at the surface of the solid sphere is given by: $$V_{surface} = V(R) = -\frac{GM}{R}$$

Finding the Gravitational Potential Difference

We are asked to find the gravitational potential difference \(V_P - V_{surface}\). $$V_P - V_{surface} = V\left(\frac{R}{2}\right) - V(R)$$ Substitute the calculated values for \(V_P\) and \(V_{surface}\): $$V_P - V_{surface} = \left(-\frac{11GM}{8R}\right) - \left(-\frac{GM}{R}\right)$$ $$V_P - V_{surface} = -\frac{11GM}{8R} + \frac{GM}{R}$$ To combine these terms, we find a common denominator, which is \(8R\): $$V_P - V_{surface} = -\frac{11GM}{8R} + \frac{8GM}{8R}$$ $$V_P - V_{surface} = \frac{-11GM + 8GM}{8R}$$ $$V_P - V_{surface} = \frac{-3GM}{8R}$$ The gravitational potential difference between point P and the surface is \(-\frac{3GM}{8R}\).

Summary of Gravitational Potential Difference Calculation

By calculating the gravitational potential at the point inside the solid sphere (\(r=R/2\)) and subtracting the gravitational potential at the surface (\(r=R\)), we found the gravitational potential difference. The potential inside depends on the distance from the center using the specific formula for a solid sphere, while the potential on the surface uses the standard formula. The resulting gravitational potential difference is \(-\frac{3GM}{8R}\).

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Important Questions from Gravitational potential energy

  1. A satellite of mass m orbits around earth in an elliptic trajectory of semi-major axis a. At a radial distance r = r 0, measured from the centre of the earth, the kinetic energy is equal to half the magnitude of the total energy. If M denotes the mass of the earth and the total energy is \( - \frac{{{\rm{GMm}}}}{{{\rm{2a}}}}\) , the value of r 0/ a is nearest to

  2. Mass of uniform circular ring is M and its radius is R. Find the maximum intensity of gravitation field on the axis of the ring

  3. The work done to raise a mass $m$ from the surface of the Earth to a height $h$, which is equal to twice the radius of the Earth $R$, is:
  4. Mass of the earth is M and its radius is R. An object of mass m is placed on the surface of earth. Find the work done in lifting the object through a height \(\frac{R}{2}\) above the surface of earth.

  5. For an object in gravitational field, the gravitational potential is the same at two points \(A\) and \(B\), but the gravitational field is not the same at these two points. Which one of the following statements is correct?
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