A Bipolar Junction Transistor (BJT) is a type of transistor used in electronic circuits for amplification, switching, and signal modulation. It consists of three doped semiconductor regions: two differently doped regions, referred to as the emitter and collector, and a moderately doped region in between, called the base. There are two main types of BJTs: NPN (negative-positive-negative) and PNP (positive-negative-positive), which refer to the arrangement of the doping types.
Here's a step-by-step explanation of the operation of an NPN BJT:
Biasing: Biasing refers to applying external voltages to the different terminals of the BJT to create specific operating conditions. In the case of an NPN transistor, you typically apply a positive voltage to the collector and a lower positive voltage to the base. The emitter is typically grounded.
Emitter-Base Junction (Forward Bias): The emitter-base junction is forward-biased, meaning a small voltage is applied across it such that the emitter is at a higher potential than the base. This biasing allows current to flow from the emitter to the base region.
Base Region: The base region is very thin and lightly doped compared to the emitter and collector. Because of its thinness and light doping, only a small number of charge carriers (electrons) flow from the emitter to the base.
Base Current: The small current flowing through the emitter-base junction is known as the base current (Ib).
Base-Collector Junction (Reverse Bias): The base-collector junction is reverse-biased, meaning a voltage is applied across it in a way that the collector is at a higher potential than the base. This biasing prevents significant current flow from the collector to the base region.
Collector Region: The collector region is heavily doped compared to the base and is larger in size. Due to the reverse biasing of the base-collector junction, it only allows a small leakage current (known as the collector current, Ic) to flow from the collector to the base region.
Transistor Action: The small base current (Ib) controls the much larger collector current (Ic). This relationship is the key principle behind the amplification capability of the BJT. A small change in the base current can lead to a significant change in the collector current.
Amplification: When a small AC signal is applied to the base-emitter junction, it causes variations in the base current. These variations are then amplified as changes in the collector current according to the transistor's current amplification factor (β or hfe).
Operating Modes: The BJT operates in three main modes:
Active Mode: The transistor is biased such that it's operating in the linear region, allowing amplification.
Saturation Mode: The transistor is biased to allow maximum current flow from collector to emitter. This is often used for switching applications.
Cutoff Mode: The transistor is biased to prevent any significant current flow from collector to emitter. It's effectively off.
In summary, a BJT operates by using a small current to control a larger current, making it a versatile component in electronic circuits for amplification and switching.