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Radiology => Electromagnetic Radiation => Photoelectric Effect
Photoelectric Effect
Photoelectric Effect, formation and liberation of electrically charged particles in matter when it is irradiated by light or other electromagnetic radiation. The term photoelectric effect designates several types of related interactions. In the external photoelectric effect, electrons are liberated from the surface of a metallic conductor by absorbing energy from light shining on the metal's surface. The effect is applied in the photoelectric cell, in which the electrons liberated from one pole of the cell, the photocathode, migrate to the other pole, the anode, under the influence of an electric field.
Study of the external photoelectric effect played an important role in the development of modern physics. Experiments beginning in 1887 showed that the external photoelectric effect had certain qualities that could not be explained by the theories of that time, in which light and all other electromagnetic radiation was considered to behave like waves. For example, as the light shining on a metal becomes increasingly intense, the classical wave theory of light suggests that the electrons that absorb the light will be liberated from the metal with more and more energy. However, experiments showed that the maximum possible energy of the ejected electrons depends only on the frequency of the incident light, and is independent of the light's intensity.
In 1905, in an effort to explain how the external photoelectric effect occurs, Albert Einstein suggested that light could be considered to behave like particles in some instances, and that the energy of each light particle, or photon, depends only on the wavelength of the light. To explain the external photoelectric effect, he envisioned light as a collection of projectiles hitting the metal. A free electron in the metal that is struck by a photon absorbs the photon's energy. If the photon is sufficiently energetic, the electron is dislodged from the metal. Einstein's theory explained many features of the external photoelectric effect, including why the maximum energy of electrons ejected from a metal is independent of the intensity of the incident light. According to his theory, the maximum energy of a dislodged electron depends only on the energy with which a photon strikes the electron; the photon's energy, however, has nothing to do with the light intensity, because intensity only measures the number of photons striking the metal. The photon's energy, and thus the maximum possible energy of a dislodged electron, depends only on the light's frequency. Einstein's theory was later verified through further experimentation. His explanation of the photoelectric effect, with its demonstration that electromagnetic radiation can behave like a collection of particles in some situations, contributed to the development of quantum theory.
The term photoelectric effect can also refer to three other processes: photoionization, photoconduction, and the photovoltanic effect. Photoionization is the ionization of a gas by light or other electromagnetic radiation; the photons must possess enough energy to detach one or more outer electrons from the gas atoms. In photoconduction, electrons in crystalline matter, by absorbing energy from photons, are brought to the range of energy levels at which they can move freely to conduct electricity. In the photovoltaic effect, photons create electron-hole pairs in semiconducting materials (see Semiconductor). In a transistor, this effect causes the formation of an electric potential across the junction between two different semiconductors in the transistor.
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