Advantages of Bundled Conductors
Bundled Conductors Used in Transmission Line
Bipolar Junction Transistor or BJT | N-P-N or P-N-P Transistor Application Theory Biasing Amplifier
Applications of Bipolar Junction Transistor or BJT | History of BJT
Biasing of Bipolar Junction Transistor | BJT or Bipolar Transistor Biasing
JFET or Junction Field Effect Transistor
Questions on JFET or Junction Field Effect Transistor
DIAC Construction Operation and Applications of DIAC
Transistor as a Switch
Application of Field Effect Transistor
Types of Transistors
n-channel JFET and p-channel JFET
Op-amp | Working Principle of Op-amp
Amplifier Gain | Decibel or dB Gain
Integrated Circuits | Types of IC
Regulated Power Supply
Laser | Types and Components of Laser
Mobility of Charge Carrier
What are Photo Electrons?
Electron volt or eV
Energy Quanta | Development of Quantum Physics
Wave Particle Duality Principle
Heisenberg Uncertainty Principle
Schrodinger Wave Equation and Wave Function
Cyclotron Basic Construction and Working Principle
Diode | Working Principle and Types of Diode
What is Zener Diode?
Application of Zener Diode
Vacuum Diode History Working Principle and Types of Vacuum Diode
p-n Junction Diode and Characteristics of p-n Junction
Full Wave Diode Rectifier
Half Wave Diode Rectifier
P-I-N Photodiode | Avalanche Photo Diode
LED or Light Emitting Diode
Tunnel Diode and its Applications
Full Wave Rectifiers
MOSFET | Working Principle of p-channel n-channel MOSFET
MOS Capacitor | MOS Capacitance C V Curve
Applications of MOSFET
MOSFET as a Switch
Diode Bridge Rectifier
Theory of Semiconductor
Energy Bands of Silicon
Donor and Acceptor Impurities in Semiconductor
Conductivity of Semiconductor
Current Density in Metal and Semiconductor
Intrinsic Silicon and Extrinsic Silicon
P Type Semiconductor
N Type Semiconductor
P N Junction Theory Behind P N Junction
Forward and Reverse Bias of P N Junction
Hall Effect Applications of Hall Effect
Bipolar Junction Transistor or BJT | N-P-N or P-N-P Transistor Application Theory Biasing Amplifier
Now, in this type of transistor any one type of semiconductors is sandwiched between the other type of semiconductor. For example, an n - type can be sandwiched between two p-type semiconductors or similarly one p-type can be sandwiched between two n-type semiconductors. These are called p-n-p and n-p-n transistors respectively. We will discuss about them later. Now as there are two junctions of different types of semiconductors, this is called junction transistor. It’s called “bipolar” because the conduction takes place due to both electrons as well as holes.
Definition of BJTA bipolar junction transistor is a three terminal semiconductor device consisting of two p-n junctions which is able to amplify or “magnify” a signal. It is a current controlled device. The three terminals of the BJT are the base, the collector and the emitter. A signal of small amplitude if applied to the base is available in the amplified form at the collector of the transistor. This is the amplification provided by the BJT. Note that it does require an external source of DC power supply to carry out the amplification process. The basic diagrams of the two types of bipolar junction transistors mentioned above are given below. From the above figure, we can see that every BJT has three parts named emitter, base and collector. JE and JC represent junction of emitter and junction of collector respectively. Now initially it is sufficient for us to know that emitter based junction is forward biased and collector base junctions is reverse biased. The next topic will describe the two types of this transistors.
N-P-N Bipolar Junction TransistorAs started before in n-p-n bipolar transistor one p - type semiconductor resides between two n-type semiconductors the diagram below a n-p-n transistor is shown Now IE, IC is emitter current and collect current respectively and VEB and VCB are emitter base voltage and collector base voltage respectively. According to convention if for the emitter, base and collector current IE, IB and IC current goes into the transistor the sign of the current is taken as positive and if current goes out from the transistor then the sign is taken as negative. We can tabulate the different currents and voltages inside the n-p-n transistor.
|n - p - n||-||+||+||-||+||+|
P-N-P Bipolar Junction TransistorSimilarly for p - n - p bipolar junction transistor a n-type semiconductors is sandwiched between two p-type semiconductors. The diagram of a p - n - p transistor is shown below For p-n-p transistors, current enters into the transistor through the emitter terminal. Like any bipolar junction transistor, the emitter-base junction is forward biased and the collector-base junction is reverse biased. We can tabulate the emitter, base and collector current, as well as the emitter base, collector base and collector emitter voltage for p-n-p transistors also.
|p - n - p||+||-||-||+||-||-|
Working Principle of BJTFigure shows an n-p-n transistor biased in the active region (See transistor biasing), the BE junction is forward biased whereas the CB junction is reversed biased. The width of the depletion region of the BE junction is small as compared to that of the CB junction. The forward bias at the BE junction reduces the barrier potential and causes the electrons to flow from the emitter to base. As the base is thin and lightly doped it consists of very few holes so some of the electrons from the emitter (about 2%) recombine with the holes present in the base region and flow out of the base terminal. This constitutes the base current, it flows due to recombination of electrons and holes (Note that the direction of conventional current flow is opposite to that of flow of electrons). The remaining large number of electrons will cross the reverse biased collector junction to constitute the collector current. Thus by KCL, The base current is very small as compared to emitter and collector current. Here, the majority charge carriers are electrons. The operation of a p-n-p transistor is same as of the n-p-n, the only difference is that the majority charge carriers are holes instead of electrons. Only a small part current flows due to majority carriers and most of the current flows due to minority charge carriers in a BJT. Hence, they are called as minority carrier devices.
Equivalent Circuit of BJTA p-n junction is represented by a diode. As a transistor has two p-n junctions, it is equivalent to two diodes connected back to back. This is called as the two diode analogy of the BJT.
Bipolar Junction Transistors CharacteristicsThe three parts of a BJT are collector, emitter and base. Before knowing about the bipolar junction transistor characteristics, we have to know about the modes of operation for this type of transistors. The modes are
- Common Base (CB) mode
- Common Emitter (CE) mode
- Common Collector (CC) mode
Common Base Characteristics
Input CharacteristicsFor p-n-p transistor, the input current is the emitter current (IE) and the input voltage is the collector base voltage (VCB). As the emitter - base junction is forward biased, therefore the graph of IE Vs VEB is similar to the forward characteristics of a p - n diode. IE increases for fixed VEB when VCB increases.
Output CharacteristicsThe output characteristics shows the relation between output voltage and output current IC is the output current and collector-base voltage and the emitter current IE is the input current and works as the parameters. The figure below shows the output characteristics for a p-n-p transistor in CB mode. As we know for p-n-p transistors IE and VEB are positive and IC, IB, VCB are negative. These are three regions in the curve, active region saturation region and the cut off region. The active region is the region where the transistor operates normally. Here the emitter junction is reverse biased. Now the saturation region is the region where both the emitter collector junctions are forward biased. And finally the cut off region is the region where both emitter and the collector junctions are reverse biased.
Common Emitter CharacteristicsInput characteristics IB (Base Current) is the input current, VBE (Base - Emitter Voltage) is the input voltage for CE (Common Emitter) mode. So, the input characteristics for CE mode will be the relation between IB and VBE with VCE as parameter. The characteristics are shown below The typical CE input characteristics are similar to that of a forward biased of p - n diode. But as VCB increases the base width decreases. Output Characteristics Output characteristics for CE mode is the curve or graph between collector current (IC) and collector - emitter voltage (VCE) when the base current IB is the parameter. The characteristics is shown below in the figure. Like the output characteristics of common - base transistor CE mode has also three regions named (i) Active region, (ii) cut-off regions, (iii) saturation region. The active region has collector region reverse biased and the emitter junction forward biased. For cut-off region the emitter junction is slightly reverse biased and the collector current is not totally cut-off. And finally for saturation region both the collector and the emitter junction are forward biased.
Application of BJTBJT's are used in discrete circuit designed due to availability of many types, and obviously because of its high transconductane and output resistance which is better than MOSFET. BJT's are suitable for high frequency application also. That’s why they are used in radio frequency for wireless systems. Another application of BJT can be stated as small signal amplifier, metal proximity photocell, etc.
Bipolar Junction Transistor AmplifierTo understand the concept of Bipolar Junction Transistor Amplifier, we should look through the diagram of a p-n-p transistor first.
Now as the input voltage is changed a little, say ΔVi of the emitter-base voltage changes the barrier height and the emitter current by ΔIE. This change in emitter current develops a voltage drop ΔVO across the load resistance RL, where, ΔVO = - RLΔIC ΔVO gives the output voltage of the amplifier. There is a negative sign because of the collector current gives a voltage drop across RL with polarity opposite to the reference polarity. The voltage gain AV for the amplifier is given the ratio between the output voltages ΔVO to the input voltage ΔVi, so, ΔIC / ΔIE = AI is called the current gain ratio of the transistor. From the figure diagram shown above we can see that an increase in the emitter voltage reduces the forward bias at the emitter junction thus decreases the collector current. It indicates that the output voltage and the input voltage are in phase. Now, finally the power gain Ap of the transistor is the ratio between the output power and the input power