MCQMediumJEE 2023Simple Harmonic Motion (SHM)

JEE Physics 2023 Question with Solution

A small particle of mass mm moves in such a way that its potential energy U=12mω2r2U = \frac{1}{2}m\omega^2 r^2 where ω\omega is constant and rr is the distance of the particle from origin. Assuming Bohr's quantization of momentum and circular orbit, the radius of the nnth orbit will be proportional to:

  • A

    nn

  • B

    n2n^2

  • C

    1n\frac{1}{n}

  • D

    n\sqrt{n}

Answer

Correct answer:D

Step-by-step solution

Standard Method

Given: The potential energy is U=12mω2r2U = \frac{1}{2}m\omega^2 r^2 and the motion is in a circular orbit.

Find: How the radius of the nnth orbit depends on nn.

For circular motion in the potential U=12mω2r2U = \frac{1}{2}m\omega^2 r^2, the force is obtained from the potential:

F=dUdr=mω2rF = -\frac{dU}{dr} = -m\omega^2 r

So the required centripetal force is

mv2r=mω2rm\frac{v^2}{r} = m\omega^2 r

This gives

v=ωrv = \omega r

Using Bohr’s postulate for angular momentum,

L=mvr=nh2πL = mvr = \frac{nh}{2\pi}

Substitute v=ωrv = \omega r:

m(ωr)r=nh2πm(\omega r)r = \frac{nh}{2\pi} mωr2=nh2πm\omega r^2 = \frac{nh}{2\pi}

Hence,

r2nr^2 \propto n

Therefore,

rnr \propto \sqrt{n}

Therefore, the radius of the nnth orbit is proportional to n\sqrt{n}. The correct option is D.

Direct Relation

Given: U=12mω2r2U = \frac{1}{2}m\omega^2 r^2 and Bohr quantization applies.

Find: The dependence of rr on nn.

From the harmonic oscillator type potential, circular motion implies v=ωrv = \omega r. Then angular momentum becomes

L=mvr=mωr2L = mvr = m\omega r^2

Bohr quantization gives

L=nh2πL = \frac{nh}{2\pi}

So directly,

mωr2nm\omega r^2 \propto n

which gives

rnr \propto \sqrt{n}

Common mistakes

  • Using Bohr quantization as mv=nh2πmv = \frac{nh}{2\pi} instead of angular momentum quantization. This is wrong because Bohr’s postulate applies to mvrmvr, not linear momentum. Always quantize L=mvrL = mvr.

  • Not deriving the force from the given potential energy. This is wrong because the relation between vv and rr comes from F=dUdrF = -\frac{dU}{dr}. First obtain the restoring force, then apply circular motion.

  • Concluding rnr \propto n after seeing LnL \propto n. This is wrong because here L=mωr2L = m\omega r^2, so angular momentum is proportional to r2r^2, not rr. Therefore solve for rr carefully.

Practice more Simple Harmonic Motion (SHM) questions

Get unlimited AI-adaptive practice, mastery tracking, and an AI tutor that explains every step — free to start.

Related questions