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Question #43613

Difficulty: 8/10 | 🟢 Free

The Question

A hypothetical nucleus AA at rest undergoes a transition to a ground state nucleus BB, emitting a single photon. The rest mass energy of nucleus AA is MAc2=500 MeVM_A c^2 = 500 \text{ MeV} and the rest mass energy of nucleus BB is MBc2=300 MeVM_B c^2 = 300 \text{ MeV}.

The emitted photon is then incident on a free atom CC, initially at rest, with rest mass energy MCc2=300 MeVM_C c^2 = 300 \text{ MeV}. The photon is completely absorbed, ejecting an electron and leaving behind an ion C′C' with rest mass energy MC′c2=360 MeVM_{C'} c^2 = 360 \text{ MeV}.

Assume the ejected electron is ultra-relativistic and can be treated as effectively massless such that its kinetic energy KeK_e and momentum pep_e are related by Ke≈pecK_e \approx p_e c. Assuming all motion occurs in one dimension, what is the maximum possible kinetic energy of the ejected electron?

Options

  • A.

    94 MeV94 \text{ MeV}

  • B.

    100 MeV100 \text{ MeV}

  • C.

    134 MeV134 \text{ MeV}

  • D.

    140 MeV140 \text{ MeV}

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How the Examiner Thinks

Multi-Concept_Bridge

Master problems that require linking physics and math concepts to solve complex competitive questions.

Concepts Behind This Question

Einstein's Photoelectric Equation|Nuclear Fission Energy Balance|Photon Neutrality

Why This Question Is Tricky

Common Mistakes

This question tests the intersection of Special Relativity and Quantum Mechanics, specifically targeting the 'Photon Neutrality / Momentum Transfer' trap.

A common student mistake is to calculate the photon energy simply as the mass defect (Δmc2=200 MeV\Delta m c^2 = 200 \text{ MeV}) and the effective work function as the rest mass difference of the atom and ion (360−300=60 MeV360 - 300 = 60 \text{ MeV}), leading directly to the trap answer of 140 MeV140 \text{ MeV}.

This fundamentally violates the conservation of momentum.

Because the photon carries momentum, the emitting nucleus must recoil, carrying away kinetic energy and red-shifting the emitted photon.

Similarly, during absorption by a free atom, the resulting ion must recoil to conserve momentum, which effectively increases the energy required to eject the electron.

Students must apply exact relativistic invariant mass equations to account for recoil in both the emission and absorption phases.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterDual Nature of Radiation and Matter - Class 12
ConceptEinstein's Photoelectric Equation
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree