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Question #43758

Difficulty: 8/10 | 🟢 Free

The Question

In a photoelectric experiment, an emitter plate at x=0x=0 is illuminated by light of frequency ff. The work function of the emitter is Φ\Phi (where hf>Φhf > \Phi). A collector plate is located at x=dx=d. Consider an electron emitted at t=0t=0 with the maximum possible kinetic energy, traveling directly along the xx-axis towards the collector. The potential difference V(t)=Vcollector−VemitterV(t) = V_{\text{collector}} - V_{\text{emitter}} is initially zero. At a time t0=d3m2(hf−Φ)t_0 = \frac{d}{3} \sqrt{\frac{m}{2(hf - \Phi)}} (where mm is the mass of the electron), the potential difference is instantaneously switched to a constant positive value V0V_0, and remains V0V_0 thereafter. Assuming the electric field between the plates is always spatially uniform, what is the kinetic energy of this electron at the instant it reaches the collector?

Options

  • A.

    hf−Φ+eV0hf - \Phi + e V_0

  • B.

    hf−Φ+23eV0hf - \Phi + \frac{2}{3} e V_0

  • C.

    hf−Φ+13eV0hf - \Phi + \frac{1}{3} e V_0

  • D.

    hf−Φhf - \Phi

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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

Instantaneous Nature|Potential Energy Reference|Integration

Why This Question Is Tricky

Common Mistakes

Students typically view photoelectric emission as a steady-state process, applying the standard equation Kmax=hf−Φ+eVK_{max} = hf - \Phi + eV by simply using the potential difference at the time of arrival.

This assumes the electric field is conservative over the entire trajectory.

However, when the potential field V(t)V(t) is time-varying, the electric field is non-conservative, and the total energy of the electron is not constant.

The trap lies in failing to recognize that the work done on the electron must be calculated by integrating the instantaneous force over the actual path (∫Fdx\int F dx).

By switching the potential while the electron is in transit, the problem forces students to track the exact position of the electron at the moment the field changes, effectively combining quantum physics with time-dependent kinematics.

Quick Facts About This Question

Question Information

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