The width of the space charge region $W$ in a pn junction is given by the formula:
$W = \sqrt{\frac{2 \epsilon V_{bi}}{q} \left( \frac{1}{N_A} + \frac{1}{N_D} \right) }$
where $\epsilon$ is the permittivity, $V_{bi}$ is the built-in voltage, and $N_A$ and $N_D$ are the doping concentrations. Substituting the values:
$W \approx 9.51 \ \mu \text{m}$
| LIST I | LIST II | ||
|---|---|---|---|
| A. | Bipolar npn transistor operate in the cut-off mode. | I. The base-emitter is reverse biased and | |
| B. | Bipolar npn transistor operate in the saturation mode. | II. Both the base-emitter and base | |
| C. | Bipolar npn transistor operate in the inverse active mode. | III. The base-emitter is forward biased | |
| D. | Bipolar npn transistor operate in the forward active mode. | IV. Both the base-emitter and bas |
| LIST I | LIST II |
|---|---|
| A. Maxwell's First Equation | I. Modified Ampere's Law |
| B. Maxwell's Second Equation | II. Faraday's Laws of Electromagnetic Induction |
| C. Maxwell's Third Equation | III. Gauss Law in Electrostatics |
| D. Maxwell's Fourth Equation | IV. Gauss Law in Magnetostatics |