MCQMediumJEE 2025Kinetic Energy & Work-Energy Theorem

JEE Physics 2025 Question with Solution

A small mirror of mass mm is suspended by a massless thread of length ll. Then the small angle through which the thread will be deflected when a short pulse of laser of energy EE falls normal on the mirror ( c=c= speed of light in vacuum and g=g= acceleration due to gravity).

  • A

    θ=3E4mcgl\theta=\frac{3 \mathrm{E}}{4 \mathrm{mc} \sqrt{g l}}

  • B

    θ=Emcgl\theta=\frac{\mathrm{E}}{\mathrm{mc} \sqrt{\mathrm{g} l}}

  • C

    θ=E2mcgl\theta=\frac{\mathrm{E}}{2 \mathrm{mc} \sqrt{\mathrm{gl}}}

  • D

    θ=2Emcgl\theta=\frac{2 \mathrm{E}}{\mathrm{mc} \sqrt{\mathrm{gl}}}

Answer

Correct answer:D

Step-by-step solution

Standard Method

Given: A small mirror of mass mm is suspended by a massless thread of length ll. A short laser pulse of energy EE falls normally on the mirror.

Find: The small angular deflection θ\theta of the thread.

For complete reflection, the force due to the laser beam is

F=2Pc=2cdEdtF = \frac{2P}{c} = \frac{2}{c} \frac{dE}{dt}

Hence, the impulse delivered to the mirror is

m(V0)=Fdt=2cdE=2Ecm(V-0) = \int F \, dt = \frac{2}{c} \int dE = \frac{2E}{c}

So the speed acquired by the mirror is

V=2EmcV = \frac{2E}{mc}

At the maximum deflection, the initial kinetic energy converts into gravitational potential energy:

12mV2=mgl(1cosθ)\frac{1}{2} mV^2 = mgl(1-\cos\theta)

For small angle deflection,

1cosθθ221-\cos\theta \approx \frac{\theta^2}{2}

Therefore,

12mV2=mgl(θ22)\frac{1}{2} mV^2 = mgl\left(\frac{\theta^2}{2}\right)

Substituting V=2EmcV = \frac{2E}{mc},

12m(4E2m2c2)=mgl(θ22)\frac{1}{2} m \left(\frac{4E^2}{m^2c^2}\right) = mgl\left(\frac{\theta^2}{2}\right) 2E2mc2=mglθ22\frac{2E^2}{mc^2} = \frac{mgl\theta^2}{2} θ2=4E2m2c2gl\theta^2 = \frac{4E^2}{m^2c^2gl} θ=2Emcgl\theta = \frac{2E}{mc\sqrt{gl}}

Therefore, the small angular deflection is 2Emcgl\frac{2E}{mc\sqrt{gl}}. The correct option is D.

Energy Conversion View

Given: A mirror of mass mm hangs as a pendulum of length ll, and a laser pulse of energy EE is reflected normally from it.

Find: The small angular deflection θ\theta.

When light reflects from a mirror, the momentum transferred is

Δp=2Ec\Delta p = \frac{2E}{c}

Hence the mirror gets horizontal momentum

p=2Ecp = \frac{2E}{c}

and corresponding speed

v=pm=2Emcv = \frac{p}{m} = \frac{2E}{mc}

As the mirror rises through a small angle, all of this kinetic energy changes into potential energy:

12mv2=mgl(1cosθ)\frac{1}{2}mv^2 = mgl(1-\cos\theta)

Using the small angle approximation,

cosθ1θ22\cos\theta \approx 1-\frac{\theta^2}{2}

so

1cosθθ221-\cos\theta \approx \frac{\theta^2}{2}

Thus,

12mv2=mglθ22\frac{1}{2}mv^2 = mg l\frac{\theta^2}{2}

Now substitute

v2=4E2m2c2v^2 = \frac{4E^2}{m^2c^2}

Then

12m(4E2m2c2)=mglθ22\frac{1}{2}m\left(\frac{4E^2}{m^2c^2}\right) = mg l\frac{\theta^2}{2} 2E2mc2=mglθ22\frac{2E^2}{mc^2} = mg l\frac{\theta^2}{2} θ2=4E2m2glc2\theta^2 = \frac{4E^2}{m^2glc^2}

Taking the positive root,

θ=2Emcgl\theta = \frac{2E}{mc\sqrt{gl}}

Therefore, the correct option is D.

Common mistakes

  • Using momentum transfer as Ec\frac{E}{c} instead of 2Ec\frac{2E}{c}. This is wrong because the light is reflected normally, so the change in momentum is doubled. Use the reflected-light result for a mirror.

  • Equating the kinetic energy to mglθmgl\theta instead of mgl(1cosθ)mgl(1-\cos\theta). This is wrong because the rise in height of the pendulum bob is geometric, not linear in θ\theta. First write the exact height change, then apply the small-angle approximation.

  • Applying the small-angle approximation incorrectly as 1cosθθ1-\cos\theta \approx \theta. This is wrong because for small angles, 1cosθθ221-\cos\theta \approx \frac{\theta^2}{2}. Use the quadratic approximation before solving for θ\theta.

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