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A Bipolar Junction Transistor (BJT) is a versatile component in electronics, functioning in four distinct modes based on the biasing of its junctions:…
A bipolar junction transistor has four modes of operation, depending upon the voltage polarities at the emitter-base junction and the collector-base junction.
In the active mode, the emitter-base junction is forward-biased, allowing electron injection from the emitter to the base. The base-collector junction is reverse-biased, blocking the flow of majority carriers.
In this mode, the transistor operates as an amplifier, with a small base current controlling a larger collector current.
In the saturation mode, both junctions are forward-biased. This mode corresponds to a small biasing voltage and a large output current, effectively acting as a closed switch.
The cut-off mode occurs when both junctions are reverse-biased, resulting in no current flow between the terminals. The transistor acts as an open switch.
In the inverted mode, the emitter-base junction is reverse-biased, while the collector-base junction is forward-biased. It is often called the inverted active mode, where the collector becomes the emitter and vice versa.
This mode has lower current gain due to reduced "emitter efficiency" caused by lower collector doping compared to base doping.
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Q1: What happens to the junctions in a BJT during active mode?
In active mode, the emitter-base junction is forward-biased, allowing electrons to be injected from the emitter to the base. Simultaneously, the base-collector junction is reverse-biased, blocking majority carriers. This configuration enables the transistor to function as an amplifier, where a small base current controls a significantly larger collector current.
Q2: How does a BJT behave when operating in saturation mode?
In saturation mode, both the emitter-base and base-collector junctions are forward-biased. The transistor acts as a closed switch with minimal biasing voltage and maximum output current. This mode is essential for switching operations where the transistor must conduct high current across its terminals.
Q3: What is the difference between cut-off and active modes in a BJT?
In cut-off mode, both junctions are reverse-biased, resulting in zero current flow and acting as an open switch. Active mode, by contrast, has a forward-biased emitter-base junction and reverse-biased collector-base junction, enabling amplification. Cut-off mode is critical in digital circuits for representing an 'off' state.
Q4: Why does inverted mode have lower current gain than active mode?
In inverted mode, the collector-base junction is forward-biased while the emitter-base junction is reverse-biased, reversing the roles of collector and emitter. Current gain is reduced due to lower emitter efficiency, caused by the collector's lower doping levels compared to the base. This asymmetry in doping concentrations limits the transistor's amplification capability.
Q5: What junction biasing conditions define each BJT operating mode?
A BJT's operating mode depends on emitter-base and collector-base junction biasing. Active mode requires forward-biased emitter-base and reverse-biased collector-base junctions. Saturation has both forward-biased; cut-off has both reverse-biased. Inverted mode features reverse-biased emitter-base and forward-biased collector-base junctions, reversing normal transistor operation.
Q6: How is a BJT used as a switch in saturation and cut-off modes?
In saturation mode, the transistor conducts maximum current, functioning as a closed switch for 'on' states. In cut-off mode, no current flows, acting as an open switch for 'off' states. These two modes enable BJTs to perform digital switching operations, making them essential components in logic circuits and power switching applications.
Q7: What role does electron injection play in BJT amplification?
During active mode, the forward-biased emitter-base junction enables electron injection from the emitter into the base region. These injected electrons are collected at the reverse-biased collector-base junction, creating a collector current much larger than the base current. This electron injection mechanism is fundamental to the transistor's amplification capability and small signal analysis of BJT amplifiers.