27 Jul 2025

BJT Operation, Current Flow, and Regions

npn and pnp transistor structure, carrier transport, terminal currents, and active, cutoff, and saturation regions.

bsc semester-iv mj-7 semiconductor-devices bjt transistor-operation

A bipolar junction transistor has two p-n junctions sharing a thin base. In an npn device the emitter is heavily doped n-type, the base is thin and lightly doped p-type, and the collector is moderately doped n-type with a larger area for voltage and heat handling. A pnp device reverses every semiconductor type and operating polarity.

Forward-active npn transport

Define

\[V_{BE}=V_B-V_E, \qquad V_{BC}=V_B-V_C.\]

Forward-active operation has the emitter-base junction forward biased, $V_{BE}>0$, and the base-collector junction reverse biased, $V_{BC}<0$. The precise forward voltage is current- and temperature-dependent; $0.6$–$0.8\,\mathrm V$ is only a common silicon range, not a mathematical boundary.

Forward-active npn transport. A heavily doped emitter injects electrons through the thin base; most reach the reverse-biased collector junction and only a small fraction recombines in the base.

The editable source is bjt-operation.tex.

Electrons injected from the emitter become minority carriers in the base. Because the neutral base width is much smaller than their diffusion length, most diffuse to the collector depletion layer and are swept into the collector. The smaller recombination fraction must be replaced through the base terminal and forms base current. Hole injection from base to emitter is kept small by the emitter’s much heavier doping.

For an npn transistor, conventional $I_C$ and $I_B$ enter collector and base while $I_E$ leaves the emitter. Using positive current magnitudes,

\[\boxed{I_E=I_C+I_B}.\]

The common-base transport factor is

\[\alpha_F=\frac{I_C}{I_E}, \qquad 0<\alpha_F<1,\]

when leakage is neglected. Efficient emitter injection and little base recombination make $\alpha_F$ close to unity. The corresponding common-emitter gain is

\[I_C\simeq\beta_F I_B, \qquad \beta_F=\frac{\alpha_F}{1-\alpha_F}.\]

These are operating-point parameters, not universal material constants.

Operating regions

The junction biases determine the region for an npn transistor:

Region	Emitter-base junction	Base-collector junction	Behaviour
Cutoff	reverse or not appreciably forward biased	reverse biased	$I_B\simeq0$ and $I_C$ is leakage-scale
Forward active	forward biased	reverse biased	$I_C\simeq\beta_FI_B$; amplification region
Saturation	forward biased	forward biased	both junctions inject; $I_C$ is circuit-limited
Reverse active	reverse biased	forward biased	emitter and collector exchange roles; gain is usually lower

In saturation, increasing $I_B$ no longer produces the active-region value $\beta_FI_B$ because the external collector circuit limits current. $V_{CE}$ then approaches a small positive $V_{CE(sat)}$ for npn operation rather than becoming exactly zero.

For a pnp transistor, holes are the principal injected carriers. Conventional currents and all voltage polarities reverse: forward-active operation requires $V_{BE}<0$ and $V_{BC}>0$. The same magnitude relations $I_E=I_C+I_B$ and $0<\alpha_F<1$ apply.