The Photoelectric Effect
The Photoelectric Effect
- Shine light on a metal and electrons fly off — but only if the light's frequency is high enough, no matter how bright it is. That stubborn fact is what proved light comes in packets.
Einstein's equation
- The is the emission of electrons from a metal surface when electromagnetic radiation is incident on it (9702/42/M/J/25 Q9(a)). One photon interacts with one electron and hands over all its energy.
Symbols
- = energy of the incoming photon (J)
- = work function — minimum energy to escape the metal (J)
- = maximum kinetic energy of the freed electron (J)
- The photon's energy pays the escape fee first; whatever is left becomes the electron's kinetic energy. The freest electrons keep the most, so the equation uses maximum KE — not an average.
- At the the KE is zero, so . Below it, no single photon has enough energy — and piling on intensity just sends more too-weak photons, so nothing escapes. This is the evidence for the photon model: energy comes in whole packets set by frequency, not spread out as a wave (9702/42/O/N/23 Q8(b)(ii)).
- Rearranged, is a straight line: plot maximum KE against frequency and the gradient is the Planck constant, the (extrapolated) intercept on the energy axis is — mind the minus sign (9702/42/O/N/23 Q8(c)). Below the line sits flat on zero (9702/41/O/N/24 Q8(c)).
Worked example
Threshold to work function to speed (2024)
A metal has threshold frequency Hz. Find its work function, then the maximum electron speed for light of Hz (9702/41/O/N/24 Q8(b)).
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Answer
Common mistake
The and threshold move together but inversely on wavelength: the metal with the smallest work function has the longest threshold wavelength (9702/42/F/M/24 Q7(c)(ii)). Reaching for the biggest number in the table gets this backwards.