E = h * c / λwhere
The maximum kinetic energy is computed as follows
Ecmax = hν - W0where
In 1887, Heinrich Hertz discovered that certain metal surfaces emit electrons when light shines upon them (called photoelectrons). This phenomenon is known as the photoelectric effect.
When the cathode of a photoelectric cell is illuminated by electromagnetic radiation, an electric current of a certain intensity (proportional to the number of the ejected electrons and which can be determined by placing an ammeter within the experimental device) is originated. The work required to release the electrons from their bonds to the metal depends on the nature of the material (binding energy). The minimum energy needed to produce photoelectric effect (that is, the energy required to extract electrons from the metal) is the extraction work (or work function). It can be written as:
W0 = h ν0; ν0 ≡ threshold frequency
When the anode is negative, due to the electrostatic interaction, it causes electrons to be repealed in such a way that only those electrons with sufficient kinetic energy to overcome the repulsive potential will be able to reach the anode. There exists a repulsive potential from which no electrons reach the anode, the so-called stopping potential, VD, which is given by:
Ec = q e-VD
In 1905, Albert Einstein explains the photoelectric effect by making the following assumptions:
E = hν
Ec = hν - W
Ec = hν - W0
λ = 2.08x10-7m
λ = 1.62x10-9m
ν = 4.2x105m/s
λ = 2.41x10-7m
v = 4.2x105m/s
V = 5.0x10-1V
ν0 = 8.44x1014Hz
V = 0.38V
ν0 = 7.55x1014Hz
E = 2.98x10-20J