Electronic Components
- Basic Electronics - Hall Effect
- Basic Electronics - Semiconductors
- Basic Electronics - Energy Bands
- Basic Electronics - Materials
Resistors
- Basic Electronics - Fixed Resistors
- Basic Electronics - Linear Resistors
- Non-linear Resistors
- Circuit Connections in Resistors
- Basic Electronics - Resistors
Capacitors
- Polarized Capacitors
- Basic Electronics - Fixed Capacitors
- Variable Capacitors
- Circuit Connections in Capacitors
- Basic Electronics - Capacitors
Inductors
- Basic Electronics - RF Inductors
- Types of Inductors
- Circuit Connections in Inductors
- Basic Electronics - Inductance
- Basic Electronics - Inductors
Transformers
- Transformer Efficiency
- Transformers based on Usage
- Types of Transformers
- Basic Electronics - Transformers
Diodes
- Optoelectronic Diodes
- Special Purpose Diodes
- Basic Electronics - Junction Diodes
- Basic Electronics - Diodes
Transistors
- Basic Electronics - MOSFET
- Basic Electronics - JFET
- Types of Transistors
- Transistor Load Line Analysis
- Transistor Regions of Operation
- Transistor Configurations
- Basic Electronics - Transistors
Basic Electronics Useful Resources
Selected Reading
- Who is Who
- Computer Glossary
- HR Interview Questions
- Effective Resume Writing
- Questions and Answers
- UPSC IAS Exams Notes
Transistor Regions of Operation
The DC supply is provided for the operation of a transistor. This DC supply is given to the two PN junctions of a transistor which influences the actions of majority carriers in these emitter and collector junctions.
The junctions are forward biased and reverse biased based on our requirement. Forward biased is the condition where a positive voltage is appped to the p-type and negative voltage is appped to the n-type material. Reverse biased is the condition where a positive voltage is appped to the n-type and negative voltage is appped to the p-type material.
Transistor biasing
The supply of suitable external dc voltage is called as biasing. Either forward or reverse biasing is done to the emitter and collector junctions of the transistor. These biasing methods make the transistor circuit to work in four kinds of regions such as Active region, Saturation region, Cutoff region and Inverse active region (seldom used). This is understood by having a look at the following table.
EMITTER JUNCTION | COLLECTOR JUNCTION | REGION OF OPERATION |
---|---|---|
Forward biased | Forward biased | Saturation region |
Forward biased | Reverse biased | Active region |
Reverse biased | Forward biased | Inverse active region |
Reverse biased | Reverse biased | Cutoff region |
Among these regions, Inverse active region, which is just the inverse of active region, is not suitable for any apppcations and hence not used.
Active region
This is the region in which transistors have many apppcations. This is also called as pnear region. A transistor while in this region, acts better as an Amppfier.
This region pes between saturation and cutoff. The transistor operates in active region when the emitter junction is forward biased and collector junction is reverse biased. In the active state, collector current is β times the base current, i.e.,
$$I_{C}:=:eta I_{B}$$
Where,
$I_{C}$ = collector current
$eta$ = current amppfication factor
$I_{B}$ = base current
Saturation region
This is the region in which transistor tends to behave as a closed switch. The transistor has the effect of its collector and Emitter being shorted. The collector and Emitter currents are maximum in this mode of operation.
The figure below shows a transistor working in saturation region.
The transistor operates in saturation region when both the emitter and collector junctions are forward biased. As it is understood that, in the saturation region the transistor tends to behave as a closed switch, we can say that,
$$I_{C}:=:I_{E}$$
Where $I_{C}$ = collector current and $I_{E}$ = emitter current.
Cutoff region
This is the region in which transistor tends to behave as an open switch. The transistor has the effect of its collector and base being opened. The collector, emitter and base currents are all zero in this mode of operation.
The following figure shows a transistor working in cutoff region.
The transistor operates in cutoff region when both the emitter and collector junctions are reverse biased. As in cutoff region, the collector current, emitter current and base currents are nil, we can write as
$$I_{C}:=:I_{E}:=:I_{B}:=:0$$
Where $I_{C}$ = collector current, $I_{E}$ = emitter current, and $I_{B}$ = base current.
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