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A fixed bias stage has \( R_{B} = 470 \ \mathrm{k\Omega} \) from a \( 12 \ \mathrm{V} \) supply. The base current is about

  • A.47 microamps
  • B.24 microamps
  • C.26 microamps, taking the thermal voltage into account as well
  • D.12 microamps, since only half the supply appears across the resistor

Answer: B

Subtracting the junction drop and dividing:

\[ \begin{aligned} I_{B} &= \frac{12 - 0.7}{470 \ \mathrm{k}} \\ &\approx 24 \ \mathrm{\mu A} \end{aligned} \]

giving about 24 microamps. With a beta of 150 that is 3.6 mA of collector current, and with a beta of 300 it would be 7.2 mA - the very spread that makes fixed bias unusable in a linear stage. The calculation is easy; the problem is what it depends on. Working one numerical case through both schemes side by side fixes the distinction better than any rule of thumb.

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