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When a particle of mass m moves on the x-axis in a potential of the form V(x) = kx2, it performs simple harmonic motion. The corresponding time period is proportional to (m/k), as can be seen easily-using dimensional analysis. However, the motion of a particle can be periodic even when its potential energy increases on both sides of x = 0 in a way different from kx2 and its total energy is such that the particle does not escape to infinity. Consider, a particle of mass m moving on the x-axis. Its potential energy is V(x) = ax4 (α > 0) for |x| near the origin and becomes a constant equal to V0 for |x| ≥ X0 (see figure).

For periodic motion of small amplitude A, the time period T of this particle is proportional to

(a) A (m/α)

(b) 1/A (m/α)

(c) A (α/m)

(d) 1/A (α/m)

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Correct Answer is: (b) 1/A (m/α)

V = αx4,  ∴ [α] = ML-2 T-2.

The only expression which has the dimension M0 L0 T is (b).

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