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Question #92558

Difficulty: 8/10 | 🟢 Free

The Question

A monochromatic light beam of wavelength λ\lambda and total power P0P_0 travels along the +y+y-direction and passes through a rectangular slit of width aa (parallel to the zz-axis). The beam falls on a detector plate of mass mm and length LzL_z (along the zz-axis) placed at a distance DD in the x−zx-z plane. Assume the optical intensity I(x)I(x) of the central diffraction maximum is uniform over its width 2x02x_0 (where x0=λDax_0 = \frac{\lambda D}{a}) and zero outside. The light generates a local surface current density on the detector given by K⃗=ηI(x)i^\vec{K} = \eta I(x) \hat{i} (in A/m), where η\eta is a positive constant. The detector is suspended by a spring of stiffness kk and is constrained to move only along the zz-axis. A non-uniform magnetic field B⃗=B0(1−x2c2)(1+βz)j^\vec{B} = B_0 \left(1 - \frac{x^2}{c^2}\right) (1 + \beta z) \hat{j} exists in the region, where B0,c,B_0, c, and β\beta are positive constants, and zz is the coordinate of the detector's center of mass. Assuming kk is sufficiently large and neglecting damping, what is the angular frequency ω\omega of the small vertical oscillations of the detector along the zz-axis?

Options

  • A.

    k−ηP0B0β(1−λ2D23a2c2)m\sqrt{\frac{k - \eta P_0 B_0 \beta \left( 1 - \frac{\lambda^2 D^2}{3 a^2 c^2} \right)}{m}}

  • B.

    k+ηP0B0β(1−λ2D23a2c2)m\sqrt{\frac{k + \eta P_0 B_0 \beta \left( 1 - \frac{\lambda^2 D^2}{3 a^2 c^2} \right)}{m}}

  • C.

    k−ηP0B0βm\sqrt{\frac{k - \eta P_0 B_0 \beta}{m}}

  • D.

    km\sqrt{\frac{k}{m}}

Check Your Answer

Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Variable_Constraint

Develop pure symbolic logic skills by mastering algebraic constraints without relying on numerical data.

Concepts Behind This Question

Resolving Power Limits|Current Density Vector|Force on Current-Carrying Loop

Why This Question Is Tricky

Examiner Levers

Variable Manipulation

Algebraic solutions only (No numbers); tests pure symbolic logic.

Difficulty Boost : +4

Common Mistakes

This question tests the student's ability to couple wave optics (Rayleigh criterion/diffraction spread) with electromagnetism (Lorentz force on a distributed surface current) and mechanics (dynamic feedback in SHM).

The primary trap lies in neglecting the feedback loop: students often assume the magnetic force only causes a static equilibrium shift and incorrectly choose k/m\sqrt{k/m}.

A secondary trap is ignoring the spatial distribution of the Airy disk/diffraction pattern, treating the beam as a point source, which misses the aperture-dependent term.

Finally, a sign error in the cross product (i^×j^\hat{i} \times \hat{j}) will lead students to incorrectly add the magnetic stiffness to the spring constant rather than subtract it.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterRay Optics and Optical Instruments - Class 12
ConceptResolving Power Limits
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree