BJT active mode

Active mode (forward-active mode) is the BJT operating region used for amplification: the emitter–base junction (EBJ) is forward-biased and the collector–base junction (CBJ) is reverse-biased. It is the BJT analogue of the MOSFET’s saturation region — the region where the device acts as a controlled current source and can amplify a small signal. (Note the unfortunate naming clash: the active BJT region corresponds to MOSFET saturation, not BJT saturation. See BJT operating modes.)

How the current gets across

Take an npn. Forward-biasing the EBJ lowers the barrier of that junction, so a large current of electrons floods from the emitter (n-type, electron-rich) into the base (p-type). Inside the base those electrons are minority carriers. The base is deliberately thin and lightly doped, so the vast majority of the injected electrons diffuse straight across it before they have a chance to recombine with the base’s holes. When they reach the edge of the depletion region around the reverse-biased CBJ, that junction’s strong electric field — pointing the right way to pull electrons toward the collector — sweeps them across and out the collector terminal. This mechanism is Minority-carrier injection.

Operating the BJT in the active region: the forward-biased EBJ sends emitter electrons across the thin base; the reverse-biased CBJ field sweeps them to the collector.

The consequence is that almost all of the emitter current reaches the collector. The collector and emitter currents differ only by the tiny fraction of carriers that recombined in the base on the way across — and that small lost fraction is the base current $i_B$. So $i_C\approx i_E$, with the difference being $i_B$.

Because the current is set by carriers crossing a forward-biased junction, the collector current depends exponentially on the EBJ forward voltage:

$i_C=I_S{e}^{v_{BE}/V_T}$

with $I_S$ the saturation current and $V_T\approx 25\text{mV}$ the Thermal voltage. This is developed fully in BJT collector current.

The current relations

Active mode is exactly the region where the three terminal currents are tied together by the gain ratios:

$i_C=\beta i_B=\alpha i_E$

• $\beta$ is the Common-emitter current gain, $i_C/i_B$, typically 50–100.
• $\alpha$ is the Common-base current gain, $i_C/i_E$, just under 1.
• KCL at the device closes the system: $i_E=i_C+i_B$.

For a large $\beta$ the three currents differ by less than 1 %, but those small differences are exactly what the amplifier exploits, so do not throw them away carelessly.

Active-mode recap: $i_C=\beta i_B=\alpha i_E$. The three currents differ by less than 1 % when β is large, but the small differences matter.

In hand analysis you assume active mode, model the EBJ as a 0.7 V drop and the collector as a $\beta i_B$ current source (the BJT large-signal model), solve, then check the assumption: the CBJ must really be reverse-biased, i.e. $V_{CE}>0.3\text{V}$ for an npn. If that fails the device is actually in BJT saturation mode and the whole analysis must be redone — see BJT DC analysis and BJT operating modes.