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PHYSICS 4340 Homework # 6
                                           Due Mar. 8

    Reading: You should finish Ch 3 through page 72 and then begin reading Chapter 7
    – band structure.

    1. An x-ray (lambda= 1.542 Å) powder photograph is made of a metallic element. The
    structure is known to be either FCC or BCC. Diffraction rings are observed at the
    following Bragg angles (theta), in degrees: 22.3, 26.0, 38.3, 46.6, 49.4, 61.2,...

    What element is it?

    Bragg Law is nλ=2dsinθ where d=2π/|G| and |G|=(2π/a)(h2+k2+l2)1/2

    So nλ = 2(2π/|G|)sinθ

    nλ 2π
              h 2 + k 2 + l 2 = sin θ
    4π a
            ⎛ nλ ⎞ 2 2
    sin θ = ⎜ ⎟ (h + k 2 + l 2 )
       2
            ⎝ 2a ⎠

    We don’t know a, but by matching the sequence of Bragg angles with the allowed values
    of h2+k2+l2, we can see if (λ/2a) is a constant (modulo n).
€
    If FCC, SG=0 unless h,k,l are all even or all odd.

    h,k,l,=111,200,220,311,222,400,331 ….

    h2+k2+l2=3,4,8,11,12,16 ….

    If BCC, SG=0 unless h+k+l is even

    h,k,l=110,200,220,310,222,312

    h2+k2+l2=2,4,8,10,12,14 …
θ           22.3,        26.0,       38.3,       46.6,      49.4,       61.2,...

       sin2θ       0.144 0.192              0.384       0.528      0.576        0.768

             sin 2 θ
                               0.048 0.048 0.048           0.048       0.048        0.048
        (h 2 + k 2 + l 2 ) fcc
             sin 2 θ
                               0.072 0.048      0.048      0.052       0.048        0.055
€       (h 2 + k 2 + l 2 ) bcc
       So the structure if FCC
€
       So letting n=0, we see (λ/2a)=0.048 for FCC. There is no nice relation for BCC. So get
       a=3.52Å, since λ =1.542 Å

       It should be Nickel.

       2. Kittel 3.1




                     L

             2k 2                  2π
       ε=                      k=      where λ = de Broglie wavelength
             2M                      λ
                                        2
                   2 ⎛ 2π ⎞  2π 2
       λ =2L, ε =     ⎜ ⎟ =         is the zero point K.E. per particle
€                 2M ⎝ 2L ⎠ 2ML2

       3. Kittel 3.5

    € a) Linear ionic crystal

       +       -           +        -       +       -    2N ions

                              Nαq 2
       Attractive term: U = −       where α=2ln2 for the 1D chain [page 71]
                               R



               €
NA             ⎛ A αq 2 ⎞
        Repulsive term: U = n or U(R) = N ⎜ n −    ⎟
                           R              ⎝ R   R ⎠

                        ∂U         ⎛ −nA αq 2 ⎞        nA αq 2
        In equilibrium,    = 0 = N ⎜ n +1 + 2 ⎟ , i.e. n +1 = 2
              €         ∂R         ⎝ R     R ⎠        R      R

         A       αq 2
               = 2
        R n +1 € nR                             €

                      ⎛ Aq 2 αq 2 ⎞      αq 2     1
€       So U(R0 ) = N ⎜     −     ⎟ = −N      (1 − ) ; linear ionic crystal: α=2ln2, so
                      ⎝ nR0   R0 ⎠       R0       n
                     2Nq 2 ln2     1
        U(R0 ) =               (1 − )
                       R0          n

€       b) Compress crystal so R0 R0(1-δ)
€
        write a Taylor series expression for

                                                              2
                                       ∂U           1       2∂ U
        U(R0 − R0δ ) = U(R0 ) − (R0δ )             + (R0δ )              − ...
                                       ∂R     R0    2        ∂R 2   R0



        The linear term vanishes at equilibrium (R=R0)

€
               ∂ 2U         ∂ ⎛ −nA αq 2 ⎞   ⎛ n(n +1)A 2αq 2 ⎞
        Now         = 0 = N ⎜ n +1 + 2 ⎟ = N ⎜          − 3 ⎟
               ∂R 2        ∂R ⎝ R   R ⎠      ⎝ R
                                                      n +2
                                                             R ⎠

                               nA αq 2
        Remembering that             =    (part a)
                               R n +1 R 2
    €
        ∂ 2U            ⎛      αq 2 2αq 2 ⎞      αq 2
                    = N ⎜(n +1) 3 − 3 ⎟ = N(n −1) 3
        ∂R 2   R0
                      €⎝       R     R ⎠         R

                                                                2
                                                      1       2∂ U
        Total work to distort= U(R0 − R0δ ) − U(R0 ) = (R0δ )
€                                                     2        ∂R 2              R0



        We want work/unit length. Here the unit length is R0.

                       €
2
                                                                                  1        2∂ U
                                                                                    (R δ )
                                                                                  2 0 ∂R 2        R0    1
        Since the total length is 2NR0, the work/unit length =                                         ≡ Cδ 2
                                                                                      2NR0              2

        ∂ 2U
        ∂R 2    αq 2
                 R0                                                 €
              =      (n −1); 	
  	
  	
  
         2NR0   2R0

        ∂ 2U               αq 2                  ∂ 2U            (n −1)q 2 log2
                       =         (n −1); C = R0 2 2          =
€       ∂R 2     R0
                           2R0 4                 ∂R     R0
                                                                      R0 2

        4. Kittel 3.7
€
        Divalent ionic crystals
        BaO in the NaCl structure. We must calculate the Madelung energies.

                               αke 2
        Ba+O-: U = −                 ; α = 1.748 (pg. 71); R 0 = 2.76Α (given)
                                R0

            −1.748(14.40eV ⋅ A)
        =                       = −9.12eV (gain)
                  2.76A
    €
                                        2
            ++    -- αk (2e)
        Ba O : U = −         = 4⋅ (−9.12) = −36.48eV (gain)
                        R0
€
     To create Ba+ and O- from Ba and O costs 5.19eV and gains us 1.5eV for a total cost of
     3.69eV.
    €
     To create Ba++ and O— from Ba+ and O- costs 9.96eV and gains us (-9.0eV), for a total
     cost of 18.96eV. Relative to Ba and O, Ba++ and O— cost us 22.65eV.
        So the Ba+ O- solid gains 9.12-3.69eV=5.43eV gain
        The Ba++O—solid gains 36.48eV-22.65eV=13.83eV gain
        Ba++O—is the stable form.

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Hw6sols

  • 1. PHYSICS 4340 Homework # 6 Due Mar. 8 Reading: You should finish Ch 3 through page 72 and then begin reading Chapter 7 – band structure. 1. An x-ray (lambda= 1.542 Å) powder photograph is made of a metallic element. The structure is known to be either FCC or BCC. Diffraction rings are observed at the following Bragg angles (theta), in degrees: 22.3, 26.0, 38.3, 46.6, 49.4, 61.2,... What element is it? Bragg Law is nλ=2dsinθ where d=2π/|G| and |G|=(2π/a)(h2+k2+l2)1/2 So nλ = 2(2π/|G|)sinθ nλ 2π h 2 + k 2 + l 2 = sin θ 4π a ⎛ nλ ⎞ 2 2 sin θ = ⎜ ⎟ (h + k 2 + l 2 ) 2 ⎝ 2a ⎠ We don’t know a, but by matching the sequence of Bragg angles with the allowed values of h2+k2+l2, we can see if (λ/2a) is a constant (modulo n). € If FCC, SG=0 unless h,k,l are all even or all odd. h,k,l,=111,200,220,311,222,400,331 …. h2+k2+l2=3,4,8,11,12,16 …. If BCC, SG=0 unless h+k+l is even h,k,l=110,200,220,310,222,312 h2+k2+l2=2,4,8,10,12,14 …
  • 2. θ 22.3, 26.0, 38.3, 46.6, 49.4, 61.2,... sin2θ 0.144 0.192 0.384 0.528 0.576 0.768 sin 2 θ 0.048 0.048 0.048 0.048 0.048 0.048 (h 2 + k 2 + l 2 ) fcc sin 2 θ 0.072 0.048 0.048 0.052 0.048 0.055 € (h 2 + k 2 + l 2 ) bcc So the structure if FCC € So letting n=0, we see (λ/2a)=0.048 for FCC. There is no nice relation for BCC. So get a=3.52Å, since λ =1.542 Å It should be Nickel. 2. Kittel 3.1 L 2k 2 2π ε= k= where λ = de Broglie wavelength 2M λ 2  2 ⎛ 2π ⎞  2π 2 λ =2L, ε = ⎜ ⎟ = is the zero point K.E. per particle € 2M ⎝ 2L ⎠ 2ML2 3. Kittel 3.5 € a) Linear ionic crystal + - + - + - 2N ions Nαq 2 Attractive term: U = − where α=2ln2 for the 1D chain [page 71] R €
  • 3. NA ⎛ A αq 2 ⎞ Repulsive term: U = n or U(R) = N ⎜ n − ⎟ R ⎝ R R ⎠ ∂U ⎛ −nA αq 2 ⎞ nA αq 2 In equilibrium, = 0 = N ⎜ n +1 + 2 ⎟ , i.e. n +1 = 2 € ∂R ⎝ R R ⎠ R R A αq 2 = 2 R n +1 € nR € ⎛ Aq 2 αq 2 ⎞ αq 2 1 € So U(R0 ) = N ⎜ − ⎟ = −N (1 − ) ; linear ionic crystal: α=2ln2, so ⎝ nR0 R0 ⎠ R0 n 2Nq 2 ln2 1 U(R0 ) = (1 − ) R0 n € b) Compress crystal so R0 R0(1-δ) € write a Taylor series expression for 2 ∂U 1 2∂ U U(R0 − R0δ ) = U(R0 ) − (R0δ ) + (R0δ ) − ... ∂R R0 2 ∂R 2 R0 The linear term vanishes at equilibrium (R=R0) € ∂ 2U ∂ ⎛ −nA αq 2 ⎞ ⎛ n(n +1)A 2αq 2 ⎞ Now = 0 = N ⎜ n +1 + 2 ⎟ = N ⎜ − 3 ⎟ ∂R 2 ∂R ⎝ R R ⎠ ⎝ R n +2 R ⎠ nA αq 2 Remembering that = (part a) R n +1 R 2 € ∂ 2U ⎛ αq 2 2αq 2 ⎞ αq 2 = N ⎜(n +1) 3 − 3 ⎟ = N(n −1) 3 ∂R 2 R0 €⎝ R R ⎠ R 2 1 2∂ U Total work to distort= U(R0 − R0δ ) − U(R0 ) = (R0δ ) € 2 ∂R 2 R0 We want work/unit length. Here the unit length is R0. €
  • 4. 2 1 2∂ U (R δ ) 2 0 ∂R 2 R0 1 Since the total length is 2NR0, the work/unit length = ≡ Cδ 2 2NR0 2 ∂ 2U ∂R 2 αq 2 R0 € = (n −1);       2NR0 2R0 ∂ 2U αq 2 ∂ 2U (n −1)q 2 log2 = (n −1); C = R0 2 2 = € ∂R 2 R0 2R0 4 ∂R R0 R0 2 4. Kittel 3.7 € Divalent ionic crystals BaO in the NaCl structure. We must calculate the Madelung energies. αke 2 Ba+O-: U = − ; α = 1.748 (pg. 71); R 0 = 2.76Α (given) R0 −1.748(14.40eV ⋅ A) = = −9.12eV (gain) 2.76A € 2 ++ -- αk (2e) Ba O : U = − = 4⋅ (−9.12) = −36.48eV (gain) R0 € To create Ba+ and O- from Ba and O costs 5.19eV and gains us 1.5eV for a total cost of 3.69eV. € To create Ba++ and O— from Ba+ and O- costs 9.96eV and gains us (-9.0eV), for a total cost of 18.96eV. Relative to Ba and O, Ba++ and O— cost us 22.65eV. So the Ba+ O- solid gains 9.12-3.69eV=5.43eV gain The Ba++O—solid gains 36.48eV-22.65eV=13.83eV gain Ba++O—is the stable form.