Photoelectric effect: Difference between revisions

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|Meaning=Any process in which [[illumination]] of a material by [[electromagnetic radiation]]  causes [[electrons]] to be separated from atoms or molecules.
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|Explanation=Photoelectric effect is often synonymous with surface photoelectric effect, "the release of electrons  by [[light]] at the boundary between a solid or liquid . . . and usually a gas" (Hughes and Dubridge  1932). The photoelectric effect was discovered in 1887 by Heinrich Hertz. The fundamental law  of photoelectricity is the Einstein law  <blockquote>[[File:ams2001glos-Pe13.gif|link=|center|ams2001glos-Pe13]]</blockquote> where ''e'' is the (maximum) [[kinetic energy]] of the emitted [[photoelectron]], &#x003bd; is the [[frequency]] of  the source of illumination, ''h'' is [[Planck's constant]], and ''p'' is the (minimum) difference between  the [[potential energy]] of an electron inside and outside the material to which it is bound. An  implicit assumption underlying this equation is that the initial kinetic energy of the electron is  negligible compared with its maximum kinetic energy. The Einstein law played a fundamental role  in establishing the [[quantum theory]] of light (Leighton 1959).<br/> Hughes, A. L., and L. A. DuBridge 1932. Photoelectric Phenomena. 1&ndash;2. <br/> Leighton, R. B. 1959. Principles of Modern Physics. 67&ndash;69.  
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== photoelectric effect ==
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<div class="definition"><div class="short_definition">Any process in which [[illumination]] of a material by [[electromagnetic radiation]]  causes [[electrons]] to be separated from atoms or molecules.</div><br/> <div class="paragraph">Photoelectric effect is often synonymous with surface photoelectric effect, &ldquo;the release of electrons  by [[light]] at the boundary between a solid or liquid . . . and usually a gas&rdquo; (Hughes and Dubridge  1932). The photoelectric effect was discovered in 1887 by Heinrich Hertz. The fundamental law  of photoelectricity is the Einstein law  <div class="display-formula"><blockquote>[[File:ams2001glos-Pe13.gif|link=|center|ams2001glos-Pe13]]</blockquote></div> where ''e'' is the (maximum) [[kinetic energy]] of the emitted [[photoelectron]], &#x003bd; is the [[frequency]] of  the source of illumination, ''h'' is [[Planck's constant]], and ''p'' is the (minimum) difference between  the [[potential energy]] of an electron inside and outside the material to which it is bound. An  implicit assumption underlying this equation is that the initial kinetic energy of the electron is  negligible compared with its maximum kinetic energy. The Einstein law played a fundamental role  in establishing the [[quantum theory]] of light (Leighton 1959).</div><br/> </div><div class="reference">Hughes, A. L., and L. A. DuBridge 1932. Photoelectric Phenomena. 1&ndash;2. </div><br/> <div class="reference">Leighton, R. B. 1959. Principles of Modern Physics. 67&ndash;69. </div><br/>
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Latest revision as of 03:07, 29 March 2024

Any process in which illumination of a material by electromagnetic radiation causes electrons to be separated from atoms or molecules.
Photoelectric effect is often synonymous with surface photoelectric effect, "the release of electrons by light at the boundary between a solid or liquid . . . and usually a gas" (Hughes and Dubridge 1932). The photoelectric effect was discovered in 1887 by Heinrich Hertz. The fundamental law of photoelectricity is the Einstein law
ams2001glos-Pe13
where e is the (maximum) kinetic energy of the emitted photoelectron, ν is the frequency of the source of illumination, h is Planck's constant, and p is the (minimum) difference between the potential energy of an electron inside and outside the material to which it is bound. An implicit assumption underlying this equation is that the initial kinetic energy of the electron is negligible compared with its maximum kinetic energy. The Einstein law played a fundamental role in establishing the quantum theory of light (Leighton 1959).
Hughes, A. L., and L. A. DuBridge 1932. Photoelectric Phenomena. 1–2.
Leighton, R. B. 1959. Principles of Modern Physics. 67–69.
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