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NCERT Exemplar · Q29

Q.Two identical heavy spheres are separated by a distance 10 times their radius. Will an object placed at the mid point of the line joining their centres be in stable equilibrium or unstable equilibrium? Give reason for your answer.

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The gravitational potential energy at the midpoint is a local maximum along the line joining the centres, so the equilibrium is unstable — a small displacement causes the object to fall toward one sphere.

Why gravitational potential energy decides stability

For any conservative force (like gravity), equilibrium occurs where the net force is zero. But the type of equilibrium — stable or unstable — depends on the shape of the potential energy curve. If the potential energy is at a minimum, a small displacement produces a restoring force (stable). If it is at a maximum, the force pushes the object further away (unstable).

Here, the object is at the midpoint of two identical spheres. By symmetry, the gravitational pulls from the two spheres cancel exactly — so the net force is zero. That is the equilibrium condition. The question is: what happens if you nudge it slightly along the line joining the centres?


Step-by-step reasoning

  1. Set up the geometry.

    Let each sphere have mass MM and radius RR. The distance between their centres is 10R10R. The midpoint is at a distance 5R5R from each centre.

  2. Write the gravitational potential energy of the object.

    For a small test mass mm placed at a distance xx from the left sphere (measured along the line joining centres), the distance to the right sphere is 10R−x10R - x. The total gravitational potential energy is

U(x)=−GMmx−GMm10R−x.U(x) = -\frac{GMm}{x} - \frac{GMm}{10R - x}.

The constant −GMm10R-\frac{GMm}{10R} from the spheres interacting with each other is irrelevant here — we only care about the shape of U(x)U(x) for the test mass.

  1. Check equilibrium at the midpoint. At x=5Rx = 5R, the derivative is

U′(x)=GMmx2−GMm(10R−x)2.U'(x) = \frac{GMm}{x^2} - \frac{GMm}{(10R - x)^2}.

Substituting x=5Rx = 5R gives U′(5R)=0U'(5R) = 0 — indeed, net force is zero.

  1. Find the second derivative to test stability.

U′′(x)=−2GMmx3−2GMm(10R−x)3.U''(x) = -\frac{2GMm}{x^3} - \frac{2GMm}{(10R - x)^3}.

At x=5Rx = 5R,

U′′(5R)=−2GMm(5R)3−2GMm(5R)3=−4GMm125R3.U''(5R) = -\frac{2GMm}{(5R)^3} - \frac{2GMm}{(5R)^3} = -\frac{4GMm}{125 R^3}.

This is negative. …

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