JEE Challenger
More from Oscillations

Particle Acceleration in Constant Potential Region

Comprehension Passage

When a particle of mass mm moves on the xx-axis in a potential of the form V(x)=kx2V(x) = kx^2, it performs simple harmonic motion. The corresponding time period is proportional to mk\sqrt{\frac{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=0x = 0 in a way different from kx2kx^2 and its total energy is such that the particle does not escape to infinity. Consider a particle of mass mm moving on the xx-axis. Its potential energy is V(x)=αx4V(x) = \alpha x^4 (α>0\alpha > 0) for ∣x∣|x| near the origin and becomes a constant equal to V0V_0 for ∣x∣≥X0|x| \ge X_0 (see figure).

Passage Diagram 0

The acceleration of this particle for ∣x∣>X0|x| > X_0 is

Options

A

proportional to V0V_0

B

proportional to V0mX0\frac{V_0}{mX_0}

C

proportional to V0mX0\sqrt{\frac{V_0}{mX_0}}

D

zero

Correct

Topics & Concepts

Step-by-Step Solution

The force F(x)F(x) acting on a particle moving along the xx-axis in a conservative force field is related to its potential energy function V(x)V(x) by the relation:
F(x)=−dV(x)dxF(x) = -\frac{dV(x)}{dx}

According to the given potential energy profile, for ∣x∣>X0|x| > X_0, the potential energy becomes constant:
V(x)=V0V(x) = V_0

Differentiating V(x)V(x) with respect to position xx in this region:
dV(x)dx=ddx(V0)=0\frac{dV(x)}{dx} = \frac{d}{dx}(V_0) = 0

Thus, the net force acting on the particle is:
F(x)=0F(x) = 0

By Newton's second law of motion, the acceleration aa of the particle is given by:
a=F(x)m=0a = \frac{F(x)}{m} = 0

Therefore, the acceleration of the particle for ∣x∣>X0|x| > X_0 is zero.

Correct Option: D