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The Franck-Hertz Experiment

In 1914 Franck and Hertz fired electrons through mercury vapour and found that the atoms would only take energy from them in one exact amount, the clearest early proof that atomic energy comes in discrete levels. The setup is simple: electrons leave the cathode, accelerate across the tube through a voltage, and are collected past a small retarding gap that only lets through electrons still carrying some energy. As long as an electron has less than the excitation energy $E_\text{exc}$ it sails through every atom elastically, losing nothing, and the collector current climbs with the voltage. But the moment its kinetic energy reaches $E_\text{exc}$ it can collide inelastically, hand exactly that lump to an atom, and drop to nearly zero, too slow to clear the retarder, so the current suddenly falls. Push the voltage higher and the electron can re-accelerate and excite a second atom, then a third, and the current dips again and again, evenly spaced by $E_\text{exc}/e$ in voltage. The scene shows it happening: electrons speed up, and wherever their energy crosses a multiple of $E_\text{exc}$ they light up a luminous layer of excited atoms, one more layer appearing with each extra step of voltage. The bottom panel is the measurement itself, the collector current against accelerating voltage, rising overall but notched at every multiple of the excitation energy. The spacing of those notches, read straight off the curve, is the excitation energy, no spectroscopy required.

Figure 1. The Franck-Hertz experiment. Top: the tube, electrons (gold) accelerating from cathode to collector, exciting atoms in luminous layers (blue) wherever their energy reaches a multiple of E_exc. Bottom: the collector current against accelerating voltage, rising but dipping at each multiple of E_exc/e, whose spacing is the excitation energy. Method: a transport simulation of acceleration and inelastic collisions. Source: Eisberg and Resnick, Quantum Physics, 2nd ed., Sec. 4.6.
11.0 V
4.9 eV

WHAT TO TRY

  • Raise the voltage slowly: each time it passes a multiple of $E_\text{exc}/e$ a new luminous layer appears and the current notches down.
  • Read the dip spacing off the bottom curve: it equals the excitation energy in volts, the experiment's whole point.
  • Change $E_\text{exc}$: the layers and the dips re-space to match, since they are set by that one energy.
  • Notice the rising trend under the dips, more of the beam is collected as the voltage grows.