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Davisson- Germer Experiment

Davisson- Germer Experiment. Prepared by: IVY CLAIRE V. MORDENO. Louis de Broglie (de broy ). Made a major advance in the understanding of atomic structure in 1924

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Davisson- Germer Experiment

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  1. Davisson-Germer Experiment Prepared by: IVY CLAIRE V. MORDENO

  2. Louis de Broglie (de broy) • Made a major advance in the understanding of atomic structure in 1924 • Nature loves symmetry. Light is dualistic in nature, behaving in some situations like waves and in others like particles. If nature is symmetric, this duality should also hold for matter. Electrons and protons, which we usually think of as particles, may in some situations behave like waves

  3. De Broglie Wave • De Broglie postulated that a free particle with rest mass , moving with nonrelativistic speed , should have a wavelength related to its momentum in exactly the same way as for a photon • The de Broglie wavelength of a particle is then • The frequency , according to de Broglie, is also related to the particle’s energy in the same way as for a photon, namely

  4. The relationships of wavelength to momentum and of frequency to energy, in de Broglie’s Hypothesis, are exactly the same for particles as for photons

  5. de Broglie’s hypothesis, almost immediately received experimental confirmation • The first direct evidence involved a diffraction experiment with electrons that was analogous to the x-ray diffraction experiments • In those experiments, atoms in a crystal act as a three-dimensional diffraction grating for x-rays. An x-ray beam is strongly reflected when it strikes a crystal at an angle that gives constructive interference among the waves scattered from the various atoms in the crystal. • These interference effects demonstrate the nature of x-rays

  6. In 1927, Clinton Davisson and Lester Germer, working at the Bell Telephone Laboratories, were studying the surface of a piece of nickel and observing how many electrons bounced off in various angles.

  7. Davisson-Germer Experiment • An apparatus similar to that used by Davisson and Germer to discover electron diffraction

  8. The specimen was polycrystalline: Like many ordinary metals, it consisted of many microscopic crystals bonded together with random orientations • The experimenters expected that even the smoothest surface attainable would still look rough to an electron and that the electron beam would be diffusely reflected, with a smooth distribution of intensity as a function of the angle θ

  9. During the experiment an accident that permitted air to enter the vacuum chamber, and an oxide film formed on the metal surface. • To remove this beam, Davisson and Germer baked the specimen in a high temperature oven, almost hot enough to melt it • Unknown to them, this had the effect of creating large single-crystal regions with planes that were continuous over the width of the electron beam

  10. When the observations were repeated, the results were quite different • Strong maxima in the intensity of the reflected electron beam occurred at specific angles in contrast to the smooth variation of intensity that had been observed before the accident

  11. The angular positions of the maxima depended on the accelerating voltage Vba used to produce the electron beam • This was not the effect that they had been looking for, but they immediately recognized that the electron beam was being diffracted • They had discovered a very direct experimental confirmation of the wave hypothesis

  12. Davisson and Germer could determine the speeds of the electrons from the accelerating voltage, so they could compute the de Broglie wavelength =

  13. The electrons were scattered primarily by the planes by atoms at the surface of crystal • Atoms in a surface plane are arranged in rows, with a distance d that can be measured by x-ray diffraction technique • These rows act like a reflecting diffraction grating • The angles of maximum reflection are given by

  14. The de Broglie wavelength of a nonrelativistic particle can be expressed in terms of the particle’s kinetic energy • Consider an electron freely accelerated from rest at point a to point b through a potential difference Vb – Va= Vba • The work done on the electron eVba equals the kinetic energy KE • Using K = we have • eVba = , • (de Broglie wavelength of an electron)

  15. References University Physics 12th Edition

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