Chapter-41 - 1577 Chapter 41 1. (a) At absolute temperature...

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Unformatted text preview: 1577 Chapter 41 1. (a) At absolute temperature T = 0, the probability is zero that any state with energy above the Fermi energy is occupied. (b) The probability that a state with energy E is occupied at temperature T is given by P E e E E kT F ( ) ( )/ = +- 1 1 where k is the Boltzmann constant and E F is the Fermi energy. Now, E – E F = 0.0620 eV and 5 ( ) / (0.0620eV) /(8.62 10 eV / K)(320K) 2.248 F E E kT-- = × = , so 2.248 1 ( ) 0.0955. 1 P E e = = + See Appendix B or Sample Problem 41-1 for the value of k . 2. We note that there is one conduction electron per atom and that the molar mass of gold is 197g mol / . Therefore, combining Eqs. 41-2, 41-3 and 41-4 leads to n = × = ×-- ( . / )( / ) ( / ) . . 19 3 10 197 590 10 3 6 3 3 28 g cm cm m g mol) / (6.02 10 mol m 23 1 3 3. (a) Eq. 41-5 gives 3/ 2 1/ 2 3 8 2 ( ) m N E E h π = for the density of states associated with the conduction electrons of a metal. This can be written 1/ 2 ( ) N E CE = where 3/ 2 31 3/2 56 3/2 3 3 3 34 3 8 2 8 2 (9.109 10 kg) 1.062 10 kg / J s . (6.626 10 J s) m C h π π-- × = = = × ⋅ × ⋅ (b) Now, 2 2 1 J 1kg m / s = ⋅ (think of the equation for kinetic energy K mv = 1 2 2 ), so 1 kg = 1 J·s 2 ·m – 2 . Thus, the units of C can be written as CHAPTER 41 1578 ( ) ( ) / / J s m J s J m 2 2 3 3/2 ⋅ ⋅ ⋅ ⋅ = ⋅----- 3 2 3 2 3 3 . This means C = × ⋅ × = × ⋅----- ( . )( . . . / 1062 10 1602 10 681 10 56 3 19 27 3 3 2 J m J / eV) m eV 3/2 3/2 (c) If E = 5.00 eV, then 27 3 3/2 1/ 2 28 1 3 ( ) (6.81 10 m eV )(5.00eV) 1.52 10 eV m . N E---- = × ⋅ = × ⋅ 4. We note that n = 8.43 × 10 28 m – 3 = 84.3 nm – 3 . From Eq. 41-9, E hc m c n F e = = ⋅ × =- 0121 0121 1240 511 10 84 3 7 0 2 2 2 3 3 3 2 3 . ( ) . ( ( . ) . / / eV nm) eV nm eV 2 where we have used 1240eV nm. hc = ⋅ 5. The number of atoms per unit volume is given by n d M = / , where d is the mass density of copper and M is the mass of a single copper atom. Since each atom contributes one conduction electron, n is also the number of conduction electrons per unit volume. Since the molar mass of copper is 63.54g / mol, A = 23 1 22 / (63.54g / mol)/(6.022 10 mol ) 1.055 10 g A M A N-- = = × = × . Thus, n = × = × = ×--- 8 96 1055 10 8 49 10 8 49 10 22 22 3 28 . . . . . g / cm g cm m 3 3 6. Let E 1 = 63 meV + E F and E 2 = – 63 meV + E F . Then according to Eq. 41-6, P e e E E kT x F 1 1 1 1 1 1 = + = +- ( )/ where x E E kT F =- ( ) / 1 . We solve for e x : e P x =- =- = 1 1 1 0 090 1 91 9 1 . . Thus, 2 1 2 ( )/ ( )/ 1 1 1 1 1 0.91, 1 1 1 (91/ 9) 1 F F E E kT E E kT x P e e e----- = = = = = + + + + where we use E 2 – E F = – 63 meV = E F – E 1 = – ( E 1 – E F ). 7. According to Eq. 41-9, the Fermi energy is given by 1579 E h m n F = F H G I K J 3 16 2 2 3 2 2 3 π / / where n is the number of conduction electrons per unit volume, m is the mass of an electron, and h is the Planck constant. This can be written E F = An 2/3 , where A h m = F H G I K J = F H G I K J × ⋅ ×...
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This note was uploaded on 08/09/2010 for the course PHY 202 101A2 taught by Professor Prof.yang during the Summer '10 term at National Taiwan University.

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Chapter-41 - 1577 Chapter 41 1. (a) At absolute temperature...

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