Bipolar junction transistor

The carrier densities are linked to the doping densities. It is less than unity due to recombination of charge carriers as they cross the base region. Conversely, the large, controlled current is referred to as the collector current because it is the only current that goes through the collector wire.

High-injection also reduces the transit time through the base, as discussed in section 5. The characteristic length, lspreading, can be obtained from a distributed model similar to that of a metal contact to a thin semiconductor layer as described in Section 3.

In other words, transistors restrict the amount of current passed according to a smaller, controlling current. Bipolar transistors are called bipolar because the main flow of electrons through them takes place in two types of semiconductor material: The functional difference between a PNP transistor and an NPN transistor is the proper biasing polarity of the junctions when operating.

Understanding how transistors function is of paramount importance to anyone interested in understanding modern electronics.

How an npn Bipolar Junction Transistor (BJT) works

The electrons in the base are called minority carriers because the base is doped p-type, which makes holes the majority carrier in the base. The recombination lifetime depends on the thermal velocity.

Base width modulation was described in section 5. This is called conventional current. High injection effects High injection effects occur in a bipolar junction transistor, just like in a p-n diode. The current gain or current transfer ratio is defined as the ratio between the emitter input current and the collector output current: Variation of the minority-carrier distribution in the base quasi-neutral region due to a variation of the base-collector voltage.

Chapter 5: Bipolar Junction Transistors

The Early voltage, VA, is also indicated on the figure. The regions of a BJT are called emitter, collector, and base.

P and N, as the main current goes from emitter to collector or vice versa. This allows thermally excited electrons to inject from the emitter into the base region. The relationships between the current and voltage of both the input and output ports are described by the following input and output characteristics.

These electrons diffuse through the base from the region of high concentration near the emitter toward the region of low concentration near the collector. This voltage variation then causes a variation of the emitter current density, especially since the emitter current density depends exponentially on the local base-emitter voltage.

The large electric field in the base-collector depletion region causes carrier multiplication due to impact ionization.

Bipolar junction transistor

Turn-on, turn-off, and storage delay[ edit ] Main article: The forward biased base-emitter BE PN-junction allows the free electrons in emitter to go through the PN-junction to arrive at the base, forming the emitter current.

The ratio of the mobility is expected to be somewhat temperature dependent due to Bipolar junction transistor different temperature dependence of the mobility in n-type and p-type material. The amount of current allowed between collector and emitter is primarily determined by the amount of current moving between base and emitter.

Temperature dependent effects in bipolar transistors The temperature dependence of bipolar transistors depends on a multitude of parameters affecting the bipolar transistor characteristics in different ways.

In this article, current arrows are shown in the conventional direction, but labels for the movement of holes and electrons show their actual direction inside the transistor. This effect is minimal in the center of the emitter-base diode and strongly increases toward the edges. The small current that controls the main current goes from base to emitter, or from emitter to base, once again depending on the kind of transistor it is PNP or NPN, respectively.

The breakdown voltage of a BJT also depends on the chosen circuit configuration: The total collector current is therefore.

The small, controlling current is usually referred to simply as the base current because it is the only current that goes through the base wire of the transistor. The base transport is more likely to be temperature dependent since it depends on the product of the diffusion constant and carrier lifetime.

However, to accurately and reliably design production BJT circuits, the voltage-control for example, Ebers—Moll model is required. It is indicated on the figure by the horizontal arrow. The onset of high injection is therefore expected if the collector current is equal or larger than: Base spreading resistance and emitter current crowding Large area bipolar transistors can have a very non-uniform current distribution due to the resistance of the base layer.

Introduction to Bipolar Junction Transistors (BJT)

Heterojunction bipolar transistors have a much higher base doping so that high-injection does not occur in such devices. The schematic symbols are shown in Figure below a and d.

Collector current is primarily limited by the base current, regardless of the amount of voltage available to push it. Bipolar transistors are so named because the controlled current must go through two types of semiconductor material: The common-base current gain is approximately the gain of current from emitter to collector in the forward-active region.The Bipolar Junction Transistor is a semiconductor device which can be used for switching or amplification In the diode tutorials we saw that simple diodes are made up from two pieces of semiconductor material to form a simple pn-junction and we.

ON Semiconductor supplies a broad portfolio of bipolar junction transistors (BJT), including audio transistors, RF transistors, darlington transistors, bias resistor transistors (BRTs), and general purpose NPN and PNP transistors.

Bipolar Junction Transistors, or BJTs, offer higher trans-conductance than MOSFETS and don't require separate gate drivers. A particular strength is that. Bipolar Transistor CHAPTER OBJECTIVES This chapter introduces the bipolar junction transistor (BJT) operation and then presents the theory of the bipolar transistor I-V characteristics, current gain, and output conductance.

High-level injection and heavy doping induced band narrowing are introduced. A variety of effects occur in bipolar transistors, which are not included in the ideal transistor model.

Bipolar Junction Transistors (BJT)

These include the base-width modulation effects and the. Chapter 4 - Bipolar Junction Transistors The invention of the bipolar transistor in ushered in a revolution in electronics. Technical feats previously requiring relatively large, mechanically fragile, power-hungry vacuum tubes were suddenly achievable with tiny, mechanically rugged, power-thrifty specks of crystalline silicon.

Bipolar junction transistor
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