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We noted in Section 12.5 (Figure 12.20) that in FeO (wüstite), the iron ions can exist in both Fe2+ and Fe3+ states. The number of each of these ion types depends on temperature and the ambient oxygen pressure. Furthermore, we also noted that in order to retain electroneutrality, one Fe2+ vacancy will be created for every two Fe3+ ions that are formed; consequently, in order to reflect the existence of these vacancies the formula for wüstite is often represented as Fe(1 – x)O, where x is some small fraction less than unity. In this nonstoichiometric Fe(1 – x)O material, conduction is electronic, and, in fact, it behaves as a p-type semiconductor—that is, the Fe3+ ions act as electron acceptors, and it is relatively easy to excite an electron from the valence band into an Fe3+ acceptor state, with the formation of a hole. Determine the electrical conductivity of a specimen of wüstite that has a hole mobility of 1.0 × 10–5 m2/V.s and for which the value of x is 0.040. Assume that the acceptor states are saturated (i.e., one hole exists for every Fe3+ ion). Wüstite has the sodium chloride crystal structure with a unit cell edge length of 0.437 nm.

Question

We noted in Section 12.5 (Figure 12.20) that in FeO (wüstite), the iron ions can exist in both Fe2+ and Fe3+ states. The number of each of these ion types depends on temperature and the ambient oxygen pressure. Furthermore, we also noted that in order to retain electroneutrality, one Fe2+ vacancy will be created for every two Fe3+ ions that are formed; consequently, in order to reflect the existence of these vacancies the formula for wüstite is often represented as Fe(1 – x)O, where x is some small fraction less than unity. In this nonstoichiometric Fe(1 – x)O material, conduction is electronic, and, in fact, it behaves as a p-type semiconductor—that is, the Fe3+ ions act as electron acceptors, and it is relatively easy to excite an electron from the valence band into an Fe3+ acceptor state, with the formation of a hole. Determine the electrical conductivity of a specimen of wüstite that has a hole mobility of 1.0 × 10–5 m2/V.s and for which the value of x is 0.040. Assume that the acceptor states are saturated (i.e., one hole exists for every Fe3+ ion). Wüstite has the sodium chloride crystal structure with a unit cell edge length of 0.437 nm.

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Solution

To determine the electrical conductivity of the wüstite specimen, we need to follow these steps:

  1. Calculate the number of Fe atoms per unit cell: Wüstite has the sodium chloride (NaCl) crystal structure. In this structure, there are 4 Fe atoms per unit cell.

  2. Determine the volume of the unit cell: The unit cell edge length is given as 0.437 nm. Volume of unit cell=(0.437×109 m)3=8.36×1029 m3 \text{Volume of unit cell} = (0.437 \times 10^{-9} \text{ m})^3 = 8.36 \times 10^{-29} \text{ m}^3

  3. Calculate the number of unit cells per cubic meter: Number of unit cells per cubic meter=18.36×1029 m3=1.20×1028 unit cells/m3 \text{Number of unit cells per cubic meter} = \frac{1}{8.36 \times 10^{-29} \text{ m}^3} = 1.20 \times 10^{28} \text{ unit cells/m}^3

  4. Calculate the number of Fe atoms per cubic meter: Number of Fe atoms per cubic meter=4×1.20×1028=4.80×1028 Fe atoms/m3 \text{Number of Fe atoms per cubic meter} = 4 \times 1.20 \times 10^{28} = 4.80 \times 10^{28} \text{ Fe atoms/m}^3

  5. Determine the number of Fe3+ ions per cubic meter: Given that x=0.040 x = 0.040 , the fraction of Fe3+ ions is 2x 2x (since one Fe2+ vacancy is created for every two Fe3+ ions). Number of Fe3+ ions per cubic meter=2x×Number of Fe atoms per cubic meter=2×0.040×4.80×1028=3.84×1027 Fe3+ ions/m3 \text{Number of Fe3+ ions per cubic meter} = 2x \times \text{Number of Fe atoms per cubic meter} = 2 \times 0.040 \times 4.80 \times 10^{28} = 3.84 \times 10^{27} \text{ Fe3+ ions/m}^3

  6. Determine the hole concentration: Since each Fe3+ ion corresponds to one hole (acceptor state is saturated), Hole concentration=3.84×1027 holes/m3 \text{Hole concentration} = 3.84 \times 10^{27} \text{ holes/m}^3

  7. Calculate the electrical conductivity: The electrical conductivity σ \sigma is given by: σ=qpμh \sigma = q \cdot p \cdot \mu_h where:

    • q q is the charge of an electron (1.6×1019 C 1.6 \times 10^{-19} \text{ C} )
    • p p is the hole concentration (3.84×1027 holes/m3 3.84 \times 10^{27} \text{ holes/m}^3 )
    • μh \mu_h is the hole mobility (1.0×105 m2/V.s 1.0 \times 10^{-5} \text{ m}^2/\text{V.s} )

    Substituting the values: σ=(1.6×1019 C)×(3.84×1027 holes/m3)×(1.0×105 m2/V.s) \sigma = (1.6 \times 10^{-19} \text{ C}) \times (3.84 \times 10^{27} \text{ holes/m}^3) \times (1.0 \times 10^{-5} \text{ m}^2/\text{V.s}) σ=6.14×103 S/m \sigma = 6.14 \times 10^{3} \text{ S/m}

Therefore, the electrical conductivity of the wüstite specimen is 6.14×103 S/m 6.14 \times 10^{3} \text{ S/m} .

This problem has been solved

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