The photoelectric effect

Light knocks electrons out of metal — but only if its wavelength is short enough, and no amount of brightness will substitute. That refusal is what made the quantum real.

Einstein (1905) · Millikan (1916)
Fowler (1931) · Berglund & Spicer (1964)
← Black-body radiation

The phototube

400 nm
1.00 W m⁻²
0.00 V

Cathode
What the apparatus does, and what the drawing leaves out 5 notes

Photocurrent against voltage the measurement

now half the intensity shorter wavelength stopping voltage

What the tube says

Stopping voltage
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Photocurrent
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    The model behind the current assumptions

    Inside the cathode

    Photoemission in three steps — excite, travel, escape. Three views: real space, energy, and momentum. The electron is not bound to any one atom to start with, so what it has to pay to get out is the work function, not the atom’s ionisation energy. And no voltage is involved — a field would make a current, which is a different thing entirely. Fire a photon and step through it.

    What just happened

      What this panel draws, and what it is not conventions & caveats

      Millikan’s line stopping voltage against frequency

      Millikan’s nine determinations, and the trap in the intercept provenance