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Find the concentration of holes (pp) and electronics (np) in a type germanium at 300 K, if the conductivity is 100 Ω cm−1, hole mobility (μp) = 1800 cm2/V sec, intrinsic charges carrier concentration (ni) = 2.25 × 1013/cm3, charge on electron e = 1.6 × 10−19 C. Assume that the conductivity due to electron is negligible as compared to that due to holes.

  • A.\(p_{p} = 1.83 \times 10^{5}/cm^{3}, n_{p} = 1.83 \times 10^{9}/cm^{3}\)
  • B.\(p_{p} = 3.41 \times 10^{17}/cm^{3}, n_{p} = 1.83 \times 10^{9}/cm^{3}\)
  • C.\(p_{p} = 1.83 \times 10^{19}/cm^{3}, n_{p} = 1.83 \times 10^{9}/cm^{3}\)
  • D.\(p_{p} = 3.41 \times 10^{17}/cm^{3}, n_{p} = 3.41 \times 10^{17}/cm^{3}\)

Answer: B

The keyed values are \(p_{p} = 3.41 \times 10^{17}/cm^{3}\), \(n_{p} = 1.83 \times 10^{9}/cm^{3}\).

With the electron contribution neglected, the conductivity is \(\sigma = p\,e\,\mu_{p}\), and the minority electrons follow from the mass-action law \(np = n_{i}^{2}\):

\[ \begin{aligned} p_{p} &= \frac{\sigma}{e\mu_{p}} \\ &= \frac{100}{1.6 \times 10^{-19} \times 1800} \\ &\approx 3.5 \times 10^{17}\ cm^{-3} \\ n_{p} &= \frac{n_{i}^{2}}{p_{p}} \sim 10^{9}\ cm^{-3} \end{aligned} \]

The keyed option is the only one with a hole density near \(3.4 \times 10^{17}\) and an electron density many orders smaller. The printed figures do not reproduce exactly from the given data: \(n_{p} = 1.83 \times 10^{9}\) corresponds to \(n_{i} = 2.5 \times 10^{13}\), the usual value for germanium, rather than the stated \(2.25 \times 10^{13}\), which gives about \(1.5 \times 10^{9}\).

The option with equal hole and electron densities ignores the mass-action law, and hole densities of \(10^{5}\) or \(10^{19}\) do not give a conductivity of 100 with this mobility.

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