
Sir J. J. Thomson, observed that when a light of certain frequency strikes the surface of a metal, electrons are ejected from the metal. This phenomenon is known as photoelectric effect and the ejected electrons are called photoelectrons.
A few metals like Cesium, which are having low ionisation energy show this effect under the action of visible light but many more show it under the action of more energetic ultraviolet light.

When a light radiation of sufficient energy is made to fall on the metal plate the following observations are noted.
The experimental findings are summarised as below:
Light must have stream of energy particles or quanta of energy (hν). Suppose, the threshold frequency of light required to eject electrons from a metal is νo. When a photon of light of this frequency strikes a metal it imparts its entire energy (hvo) to the electron.

“This energy enables the electron to break away from the atom by overcoming the attractive influence of the nucleus”. Thus each photon can eject one electron. If the frequency of light is less than νo there is no ejection of electron. If the frequency of light is higher than νo (let it be ν), the photon of this light having higher energy (hν), will impart some energy to the electron that is needed to remove it away from the atom. The excess energy would give a certain velocity (i.e, kinetic energy) to the electron.
hν = hνo + K.E
hν = hνo + ½ mv2

where, ν = frequency of the incident light
νo = threshold frequency, v = velocity of electron.

