In 1913 Bohr took Rutherford's nucleus model of the hydrogen atom as the basis for his quantized atom model (► Bohr's atomic
model; Rutherford atom). Although it was not the first, it was the first successful atom model. A year later, two Berlin experimenters,
James Franck (1882–1964) and Gustav Hertz (1887–1975), unaware of Bohr's model and its implications, performed an experiment
which later turned out to be one of its strongest corroborations. For the so-called
Franck—Hertz experiment, they were awarded the Nobel Prize for Physics in 1925. In this experiment ► electrons are ejected from a cathode,
C, into a tube filled with mercury gas (see Fig. 1). The energy of the electrons can be increased in a controllable manner
by accelerating them towards the positively charged grid,
G, through the potential difference
V
a. Electrons fly through the grid towards anode
A. Between
G and
A, a small retarding voltage,
V
r, decelerates the electrons. They will only reach the anode
A, if their energies
V exceed
V
r, where they will be recorded by the ammeter A.
Collisions between the atoms and the electrons will occur. Only electrons with sufficient energy will cause the mercury atoms
to make transitions to higher states of energy. The electrons will lose their energy to the atoms. When V
a = 4.9 V, the curve drops very sharply.