Exam 41: Conduction of Electricity in Solids

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If the density of states is N(E) and the occupancy probability is P(E), then the density of unoccupied states is:

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If E0 and ET are the average energies of the "free" electrons in a metal at 0 K and room temperature respectively, then the ratio ET/E0 is approximately:

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For a pure semiconductor the Fermi level is:

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The energy level diagram shown applies to: The energy level diagram shown applies to:

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The energy gap (in eV) between the valence and conduction bands of an insulator is of the order:

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At room temperature kT is about 0.0259 eV. The probability that a state 0.50 eV below the Fermi level is unoccupied at room temperature is:

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A donor replacement atom in silicon might have ______ electrons in its outer shell.

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Application of a forward bias to a p-n junction:

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At T = 0 K the probability that a state 0.50 eV below the Fermi level is occupied is:

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For a metal at absolute temperature T, with Fermi energy EF, the occupancy probability is given by:

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The Fermi-Dirac probability function P(E) varies between:

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The speed of an electron with energy equal to the Fermi energy for copper is on ther order of:

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"LED" stands for:

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Possible units for the density of states function N(E) are:

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In a pure metal the collisions that are characterized by the mean free time τ \tau in the expression for the resistivity are chiefly between:

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A certain material has a resistivity of 7.8 *103 Ω\Omega . m at room temperature and it decreases as the temperature is raised by 100 °\degree C. The material is most likely:

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For a pure semiconductor at room temperature the temperature coefficient of resistivity is determined primarily by:

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The contact electric field in the depletion region of a p-n junction is produced by:

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A certain metal has 5.3 *1029 conduction electrons/m3 and an electrical resistivity of 1.9 * 10-9 Ω\Omega .m.The average time between collisions of electrons with atoms in the metal is:

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When a forward bias is applied to a p-n junction the concentration of electrons on the p side:

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