Start Learning Free

Before You Begin

Question #43609

Difficulty: 8/10 | 🟢 Free

The Question

A large metallic plate lying in the xx-yy plane (z=0z=0) has a work function WW. It is illuminated by monochromatic light of photon energy EphE_{ph} (where Eph>WE_{ph} > W). Consider a photoelectron emitted from the origin with the maximum possible kinetic energy, at an angle θ\theta with the +z+z-axis. In the region z>0z > 0, a uniform electric field E⃗=E0k^\vec{E} = E_0 \hat{k} is present, which acts as a retarding field for the emitted electrons. Let z0z_0 be the maximum zz-coordinate reached by this specific electron. Suppose that exactly at the plane z=z0z = z_0, the electric field abruptly terminates, and a non-uniform magnetic field B⃗=B0(1+αz)k^\vec{B} = B_0(1 + \alpha z)\hat{k} exists for all z≥z0z \ge z_0. What is the radius of curvature of the electron's trajectory immediately after it enters the magnetic field region? (Assume mm and −e-e are the mass and charge of the electron, respectively. Neglect gravity. Let ΔE=Eph−W\Delta E = E_{ph} - W. E0,B0E_0, B_0, and α\alpha are positive constants with appropriate SI units).

Options

  • A.

    2mΔEsin⁡θeB0(1+αΔEcos⁡2θeE0)\frac{\sqrt{2m\Delta E} \sin\theta}{e B_0 \left( 1 + \frac{\alpha \Delta E \cos^2\theta}{e E_0} \right)}

  • B.

    2mΔEsin⁡θeB0(1+αΔEeE0)\frac{\sqrt{2m\Delta E} \sin\theta}{e B_0 \left( 1 + \frac{\alpha \Delta E}{e E_0} \right)}

  • C.

    2mΔEeB0(1+αΔEcos⁡2θeE0)\frac{\sqrt{2m\Delta E}}{e B_0 \left( 1 + \frac{\alpha \Delta E \cos^2\theta}{e E_0} \right)}

  • D.

    2mΔEcos⁡θeB0(1+αΔEsin⁡2θeE0)\frac{\sqrt{2m\Delta E} \cos\theta}{e B_0 \left( 1 + \frac{\alpha \Delta E \sin^2\theta}{e E_0} \right)}

Check Your Answer

Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Intuition_Breaker

Train your brain to resist "obvious" answers that are designed to deceive your intuition.

Concepts Behind This Question

Stopping Potential Independence|Non-Uniform Circular Motion|Vector Cross-Product

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to decouple the orthogonal components of a photoelectron's motion under the influence of independent electric and magnetic fields.

A common trap is assuming that the retarding electric field (which acts as a stopping potential) diminishes the electron's total kinetic energy to zero at the turning point.

Students incorrectly apply the total kinetic energy ΔE\Delta E to find both the maximum penetration depth z0z_0 and the tangential velocity vtv_t, ignoring the angular distribution of emission.

The correct framework requires recognizing that the electric field only halts the longitudinal velocity component (vzv_z), while the transverse velocity (vtv_t) remains unaffected and dictates the radius of curvature when the electron enters the magnetic field.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterDual Nature of Radiation and Matter - Class 12
ConceptStopping Potential Independence
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree