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In the photoelectric effect, what happens when light of sufficient frequency hit

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Question: In the photoelectric effect, what happens when light of sufficient frequency hits a metal surface?

Options:

  1. Electrons are emitted from the surface
  2. Photons are absorbed by the metal
  3. The metal becomes ionized
  4. Heat is generated in the metal

Correct Answer: Electrons are emitted from the surface

Solution:

When light of sufficient frequency hits a metal surface, it can provide enough energy to eject electrons from the metal.

In the photoelectric effect, what happens when light of sufficient frequency hit

Practice Questions

Q1
In the photoelectric effect, what happens when light of sufficient frequency hits a metal surface?
  1. Electrons are emitted from the surface
  2. Photons are absorbed by the metal
  3. The metal becomes ionized
  4. Heat is generated in the metal

Questions & Step-by-Step Solutions

In the photoelectric effect, what happens when light of sufficient frequency hits a metal surface?
  • Step 1: Understand that light is made up of tiny particles called photons.
  • Step 2: Know that each photon has a certain amount of energy, which depends on its frequency (how fast the light waves oscillate).
  • Step 3: Recognize that metals have electrons that are loosely bound to their atoms.
  • Step 4: Learn that if the frequency of the incoming light is high enough, the energy of the photons can overcome the attraction of the electrons to the metal.
  • Step 5: When the light hits the metal surface, the photons transfer their energy to the electrons.
  • Step 6: If the energy is sufficient, the electrons gain enough energy to break free from the metal surface.
  • Step 7: The ejected electrons are called photoelectrons.
  • Photoelectric Effect – The phenomenon where light of sufficient frequency causes the ejection of electrons from a metal surface.
  • Threshold Frequency – The minimum frequency of light required to eject electrons from a metal.
  • Photon Energy – The energy of a photon is directly proportional to its frequency, as described by the equation E = hf.
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