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Electron Thermal Conductivity in Metals

The mean free path of electron is a direct function of the electron collision frequency. Electrons can collide with other electrons, lattice, defects, grain boundaries, and surfaces. [Pg.318]

Assuming that each scattering mechanism is independent, collisional rate is the sum of the individual scattering mechanism  [Pg.319]

The collisional frequency can also be dependent on temperature. Electron-defect and electron-boundary scattering are typically independent of temperature. Debye temperature is a characteristic temperature arising in the computation of Debye specific heat. It is defined as [Pg.319]

A and B are constants and and Tf are the electron and lattice temperature, respectively. [Pg.319]


Smirnov, I.A., and V.I. Tamarchenko, 1977, Electronic Thermal Conductivity in Metals and Semiconductors (Nauka, Leningrad). In Russian. [Pg.223]


See other pages where Electron Thermal Conductivity in Metals is mentioned: [Pg.318]   


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