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Zorluk: Çok zorPhotoelectric Effect and Work Function

A clean metal surface with threshold frequency f0f_0 is illuminated by monochromatic radiation of frequency 2f02f_0 and light intensity II, causing emission of photoelectrons with maximum kinetic energy K1K_1 and stopping potential V1V_1. If the source is changed to radiate light of frequency 3f03f_0 while its intensity is simultaneously doubled to 2I2I, what are the new maximum kinetic energy K2K_2 and stopping potential V2V_2 in terms of K1K_1 and V1V_1?

  1. K2=2K1K_2 = 2K_1 and V2=2V1V_2 = 2V_1Cevap
  2. B
    K2=4K1K_2 = 4K_1 and V2=4V1V_2 = 4V_1
  3. C
    K2=4K1K_2 = 4K_1 and V2=2V1V_2 = 2V_1
  4. D
    K2=3K1K_2 = 3K_1 and V2=3V1V_2 = 3V_1

Cevap

K2=2K1K_2 = 2K_1 and V2=2V1V_2 = 2V_1
By Einstein's photoelectric law, Kmax=hfW0K_{\max} = hf - W_0. For incident frequency 2f02f_0 and work function W0=hf0W_0 = hf_0, the initial kinetic energy is K1=2hf0hf0=hf0K_1 = 2hf_0 - hf_0 = hf_0. For incident frequency 3f03f_0, the new kinetic energy is K2=3hf0hf0=2hf0=2K1K_2 = 3hf_0 - hf_0 = 2hf_0 = 2K_1. Since stopping potential is related by eVs=KmaxeV_s = K_{\max}, V2=2V1V_2 = 2V_1. Doubling the light intensity from II to 2I2I doubles the rate of photoelectron emission but does not alter maximum kinetic energy or stopping potential.

Adım Adım Çözüm

1
Apply Einstein's photoelectric equation to the initial condition.
K1=h(2f0)hf0=hf0K_1 = h(2f_0) - hf_0 = hf_0, and eV1=K1=hf0e V_1 = K_1 = hf_0.
The maximum kinetic energy is the energy of the incident photon minus the work function of the metal plate.
2
Apply Einstein's photoelectric equation to the new frequency condition.
K2=h(3f0)hf0=2hf0=2K1K_2 = h(3f_0) - hf_0 = 2hf_0 = 2K_1, and eV2=K2=2hf0=2eV1    V2=2V1e V_2 = K_2 = 2hf_0 = 2e V_1 \implies V_2 = 2V_1.
The new photon energy is 3hf03hf_0, leaving 2hf02hf_0 of excess energy as photoelectron maximum kinetic energy.
3
Evaluate the effect of doubling light intensity to 2I2I.
Light intensity has zero impact on individual photoelectron kinetic energy or stopping potential; it only increases the emission rate (saturation photocurrent).
Photoelectric emission is a one-to-one photon-electron interaction process where photon frequency dictates individual energy.

Anahtar Kavram

Independence of photoelectron kinetic energy and stopping potential from light intensity
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