Photons and the Photoelectric Effect
Light comes in quanta called photons, each of energy ( J s) and momentum . When photons hit a metal, each can release one electron if its energy exceeds the work function : . Below the threshold frequency , no electrons are emitted, however bright the light. Brighter light means more photons, so more electrons, but not faster ones.
Learning objectives
- Use , the electronvolt and .
- Describe the photoelectric effect and define threshold frequency and work function.
- Use .
- Explain the effects of frequency and intensity using the photon model.
Very bright red light shone on zinc releases no electrons, but dim ultraviolet does. How can dimmer light do more?
Core idea
Shine the brightest red lamp on a zinc plate: no electrons come out. Shine a faint ultraviolet lamp: electrons fly off instantly. Waves can't explain this. Light must arrive in packets, each with an energy set by its frequency.
. One photon frees at most one electron: . Threshold .
1. Evidence for photons
- Emission is instant, even in dim light.
- Max KE depends on frequency, not intensity.
- Intensity only changes the number of electrons per second.
- Wave theory predicts none of these.
2. Einstein's equation
- Energy delivered by one photon, all to one electron.
- At least is needed to escape; the rest is kinetic (maximum for surface electrons).
- Stopping potential just halts the fastest electrons.
- Threshold frequency.
eV.
- Goal
- Photon energy; max KE; threshold wavelength.
- Strategy
- in eV.
- ÷ .
- Stopping potential 0.67 V.
- Longer wavelengths emit nothing.
1.0 mW at 500 nm.
- Goal
- Photons per second.
- Strategy
- Power ÷ energy per photon.
- One photon.
- Rate.
Summary
- .
- .
- 1 eV J.
- Work function
- Minimum energy to free an electron.
- Photon
- Quantum of EM energy.
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