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What is the number density of conduction electrons in gold, which is a monovalent metal? Use the molar mass and density provided in Appendix F.

Short Answer

Expert verified

The number density of conduction electrons in gold is 5.90×1028m-3.

Step by step solution

01

The given data

a) The gold is monovalent element.

b) Molar mass of gold (Appendix F),A = 197 g/mol

c) Density of gold (Appendix F),d=19.3g/cm3

02

Understanding the concept of density and molar mass

Mass of one mole of a sample of element is known as Molar mass. According to Avogadro, one mole of a sample consists of6.022×1023 atoms, also known as Avogadro’s Number. Thus, if we divide the molar mass with Avogadro’s Number, we will get the mass of one atom of an element.

Formulae:

The mass of an atom, M=A/NA,whereNA=6.022×1023mol-1 (i)

The number density of conduction electrons,n=dM (ii)

d= density of the atom, M = mass of a single atom

03

Calculation of the number density of conductions electrons in gold

Since each atom contributes one conduction electron, the number of conduction electrons per unit volume should be equal to the number density of atoms of gold present in the sample.

Using equation (i) in equation (ii), the number density of the conduction electrons in gold is given as-

n=dA/NA=19.3g/cm3106cm3/m3197g/mol/6.022×1023mol-1=5.90×1028m3

Hence, the value of the number density is 5.90×1028m3.

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Most popular questions from this chapter

The occupancy probability function (Eq. 41-6) can be applied to semiconductors as well as to metals. In semiconductors the Fermi energy is close to the midpoint of the gap between the valence band and the conduction band. For germanium, the gap width is 0.67eV. What is the probability that (a) a state at the bottom of the conduction band is occupied and (b) a state at the top of the valence band is not occupied? Assume that T = 290K. (Note:In a pure semiconductor, the Fermi energy lies symmetrically between the population of conduction electrons and the population of holes and thus is at the center of the gap. There need not be an available state at the location of the Fermi energy.)

(a) Show that the slope dP/dEof Eq. 41-6 evaluated atE=EFis -1/4kT. (b) Show that the tangent line to the curve of Fig. 41-7bevaluated atE=EFintercepts the horizontal axis atE=EF+2kT.

At 1000K, the fraction of the conduction electrons in a metal that have energies greater than the Fermi energy is equal to the area under the curve of Fig. 41-8bbeyond EF divided by the area under the entire curve. It is difficult to find these areas by direct integration. However, an approximation to this fraction at any temperature T is frac=3kT2EF.

Note that frac = 0 for T = 0 K, just as we would expect. What is this fraction for copper at (a) 300 K and (b) 1000 K? For copper EF=7.0eV. (c) Check your answers by numerical integration using Eq. 41-7.

At T = 300K, how far above the Fermi energy is a state for which the probability of occupation by a conduction electron is 0.10?

Zinc is a bivalent metal. Calculate (a) the number density of conduction electrons, (b) the Fermi energy, (c) the Fermi speed, and (d) the de Broglie wavelength corresponding to this electron speed. See Appendix F for the needed data on zinc.

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