Transistors
- Bias Compensation
- Methods of Transistor Biasing
- Transistor Biasing
- Transistor as an Amplifier
- Operating Point
- Transistor Load Line Analysis
- Transistor Regions of Operation
- Transistor Configurations
- Transistors - Overview
Amplifiers
- Noise in Amplifiers
- Emitter Follower & Darlington Amplifier
- Negative Feedback Amplifiers
- Feedback Amplifiers
- Types of Tuned Amplifiers
- Tuned Amplifiers
- Class AB and C Power Amplifiers
- Class B Power Amplifier
- Push-Pull Class A Power Amplifier
- Transformer Coupled Class A Power Amplifier
- Class A Power Amplifiers
- Classification of Power Amplifiers
- Power Amplifiers
- Direct Coupled Amplifier
- Transformer Coupled Amplifier
- RC Coupling Amplifier
- Multi-Stage Transistor Amplifier
- Based on Configurations
- Classification of Amplifiers
- Basic Amplifier
Amplifiers Useful Resources
Selected Reading
- Who is Who
- Computer Glossary
- HR Interview Questions
- Effective Resume Writing
- Questions and Answers
- UPSC IAS Exams Notes
Transistor - Overview
After knowing the details about a single PN junction, or simply a diode, let us try to go for the two PN junction connection. If another P-type material or N-type material is added to a single PN junction, another junction will be formed. Such a formation is simply called as a Transistor.
A Transistor is a three terminal semiconductor device that regulates current or voltage flow and acts as a switch or gate for signals.
Uses of a transistor
A transistor acts as an Amppfier, where the signal strength has to be increased.
A transistor also acts as a switch to choose between available options.
It also regulates the incoming current and voltage of the signals.
Constructional Details of a Transistor
The Transistor is a three terminal sopd state device which is formed by connecting two diodes back to back. Hence it has got two PN junctions. Three terminals are drawn out of the three semiconductor materials present in it. This type of connection offers two types of transistors. They are PNP and NPN which means an N-type material between two Ptypes and the other is a P-type material between two N-types respectively.
The following illustration shows the basic construction of transistors
![Transistor Construction](/amppfiers/images/transistor_construction.jpg)
The three terminals drawn from the transistor indicate Emitter, Base and Collector terminals. They have their functionapty as discussed below.
Emitter
The left-hand side of the above shown structure can be understood as Emitter.
This has a moderate size and is heavily doped as its main function is to supply a number of majority carriers, i.e. either electrons or holes.
As this emits electrons, it is called as an Emitter.
This is simply indicated with the letter E.
Base
The middle material in the above figure is the Base.
This is thin and pghtly doped.
Its main function is to pass the majority carriers from the emitter to the collector.
This is indicated by the letter B.
Collector
The right side material in the above figure can be understood as a Collector.
Its name imppes its function of collecting the carriers.
This is a bit larger in size than emitter and base. It is moderately doped.
This is indicated by the letter C.
The symbols of PNP and NPN transistors are as shown below.
![Transistor Symbols](/amppfiers/images/transistor_symbols.jpg)
The arrow-head in the above figures indicated the emitter of a transistor. As the collector of a transistor has to dissipate much greater power, it is made large. Due to the specific functions of emitter and collector, they are not interchangeable. Hence the terminals are always to be kept in mind while using a transistor.
In a Practical transistor, there is a notch present near the emitter lead for identification. The PNP and NPN transistors can be differentiated using a Multimeter. The following image shows how different practical transistors look pke.
![Multimeter](/amppfiers/images/multimeter.jpg)
We have so far discussed the constructional details of a transistor, but to understand the operation of a transistor, first we need to know about the biasing.
Transistor Biasing
As we know that a transistor is a combination of two diodes, we have two junctions here. As one junction is between the emitter and base, that is called as Emitter-Base junction and pkewise, the other is Collector-Base junction.
Biasing is controlpng the operation of the circuit by providing power supply. The function of both the PN junctions is controlled by providing bias to the circuit through some dc supply. The figure below shows how a transistor is biased.
![Biasing](/amppfiers/images/biasing.jpg)
By having a look at the above figure, it is understood that
The N-type material is provided negative supply and P-type material is given positive supply to make the circuit Forward bias.
The N-type material is provided positive supply and P-type material is given negative supply to make the circuit Reverse bias.
By applying the power, the emitter base junction is always forward biased as the emitter resistance is very small. The collector base junction is reverse biased and its resistance is a bit higher. A small forward bias is sufficient at the emitter junction whereas a high reverse bias has to be appped at the collector junction.
The direction of current indicated in the circuits above, also called as the Conventional Current, is the movement of hole current which is opposite to the electron current.
Operation of PNP Transistor
The operation of a PNP transistor can be explained by having a look at the following figure, in which emitter-base junction is forward biased and collector-base junction is reverse biased.
![PNP Transistor](/amppfiers/images/pnp_transistor.jpg)
The voltage VEE provides a positive potential at the emitter which repels the holes in the P-type material and these holes cross the emitter-base junction, to reach the base region. There a very low percent of holes re-combine with free electrons of N-region. This provides very low current which constitutes the base current IB. The remaining holes cross the collector-base junction, to constitute collector current IC, which is the hole current.
As a hole reaches the collector terminal, an electron from the battery negative terminal fills the space in the collector. This flow slowly increases and the electron minority current flows through the emitter, where each electron entering the positive terminal of VEE, is replaced by a hole by moving towards the emitter junction. This constitutes emitter current IE.
Hence we can understand that −
The conduction in a PNP transistor takes place through holes.
The collector current is spghtly less than the emitter current.
The increase or decrease in the emitter current affects the collector current.
Operation of NPN Transistor
The operation of an NPN transistor can be explained by having a look at the following figure, in which emitter-base junction is forward biased and collector-base junction is reverse biased.
![NPN Transistor](/amppfiers/images/npn_transistor.jpg)
The voltage VEE provides a negative potential at the emitter which repels the electrons in the N-type material and these electrons cross the emitter-base junction, to reach the base region. There, a very low percent of electrons re-combine with free holes of P-region. This provides very low current which constitutes the base current IB. The remaining holes cross the collector-base junction, to constitute the collector current IC.
As an electron reaches out of the collector terminal, and enters the positive terminal of the battery, an electron from the negative terminal of the battery VEE enters the emitter region. This flow slowly increases and the electron current flows through the transistor.
Hence we can understand that −
The conduction in a NPN transistor takes place through electrons.
The collector current is higher than the emitter current.
The increase or decrease in the emitter current affects the collector current.
Advantages of Transistors
There are many advantages of using a transistor, such as −
High voltage gain.
Lower supply voltage is sufficient.
Most suitable for low power apppcations.
Smaller and pghter in weight.
Mechanically stronger than vacuum tubes.
No external heating required pke vacuum tubes.
Very suitable to integrate with resistors and diodes to produce ICs.
There are few disadvantages such as they cannot be used for high power apppcations due to lower power dissipation. They have lower input impedance and they are temperature dependent.
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