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Cut off wavelength of electron on lithum
Cut off wavelength of electron on lithum






With this energy absorbed, the most energetic electron is released with Kmax by overcoming the surface energy barrier or work function ϕ 0 and this is expressed as The energy absorbed by each electron in time t is given by For the sake of simplicity, the following assumptions are made.Ī) Light is absorbed in the top atomic layer of the metalī) For a given element, each atom absorbs an equal amount of energy and this energy is proportional to its cross-sectional area AĬ) Each atom gives this energy to one of the electrons. I) According to wave theory, the energy in a light wave is spread out uniformly and continuously over the wavefront. (Given : The work function for cesium is 2.14 eV and the power absorbed per unit area is 1.60×10 −6 Wm −2 which produces a measurable photocurrent in cesium.) Solution Iii) the time interval between the incidence of light and the ejection of photoelectrons is very long. Ii) K maxdoes not depend on the frequency of the incident light and

cut off wavelength of electron on lithum

I) maximum kinetic energy of the photoelectrons ( K max) depends on the intensity I of the incident light

cut off wavelength of electron on lithum cut off wavelength of electron on lithum

For the photoelectric emission from cesium, show that wave theory predicts that








Cut off wavelength of electron on lithum