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Bipolar Junction Transistor
Biasing of BJT
Current Components in a Transistor
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Applications of BJT
Transistor as a Switch
Transistor as an Amplifier
n-channel JFET and p-channel JFET
Applications of FET
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Mobility of Charge Carrier
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Electron volt or eV
Energy Quanta | Development of Quantum Physics
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Application of Zener Diode
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P Type Semiconductor
N Type Semiconductor
P N Junction
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Biasing of Bipolar Junction Transistor or BJT
Cutoff Mode of BJTThe BJT is fully off in this state. In the cutoff mode both the base emitter as well as collector base junction is reverse biased. The BJT is equivalent to an open switch in this mode.
Saturation Mode of BJTThe transistor is fully on in this state. The CB as well as BE junctions are forward biased. The BJT operates like a closed switch in the saturation mode. If a BJT is in saturation mode than it should satisfy the following condition, Where, βDC is common emitter current amplification factor or current gain.
Active Mode of BJTIn order to use the transistor as an amplifier, it must be operated in the active mode. The BE junction is forward biased whereas the CB junction is reverse biased. Figure below shows both n-p-n and p-n-p transistors biased in the active mode of operation.
Biasing Circuits of BJTTo make the Q point stable different biasing circuits are tried. The Q point is also called as operating bias point, is the point on the DC load line (a load line is the graph of output current vs. output voltage in any of the transistor configurations) which represents the DC current through the transistor and voltage across it when no ac signal is applied. The Q point represents the DC biasing condition. When the BJT is biased such that the Q point is halfway between cutoff and saturation than the BJT operates as a CLASS-A amplifier. The three circuits or biasing arrangements which are practically used are explained below.
Fixed Bias or Base BiasIn this condition a single power source is applied to the collector and base of the transistor using only two resistors. Applying KVL to the circuit,
Thus, by merely changing the value of the resistor the base current can be adjusted to the desired value. And by using the current gain (β) relationship, IC can also be found out accordingly. Hence the Q point can be adjusted just by changing the value of the resistor connected to the base.
Collector to Base BiasThis connection is mostly used to stabilize the operating point against temperature changes. In this type, the base resistor is connected to the collector instead of connecting it to the supply. So any thermal runaway will induce IR drop in the collector resistor. The base current can be derived as, If VBE kept constant and there is an increase in temperature, then the collector current increases. However, a larger collector current causes the voltage drop across the collector resistor to increase, which reduces the voltage across the base resistor. This will reduce the base current, hence resulting less collector current. Because an increase in collector current with temperature is opposed, the operating point is stable.
Self Bias or Voltage Divider BiasThe circuit diagram for self bias is shown below. This is the most widely used biasing circuit. The electrical resistances R1 and R2 form a potential divider arrangement to apply a fixed voltage to the base. Consider only the base circuit, the approximate voltage across the base is Consider only the collector circuit, the approximate emitter current will be, In the above circuit, as the emitter resistor causes ac as well as DC feedback the AC voltage gain of the amplifier is reduced. This can avoided by connecting a capacitor in parallel with the emitter resistor as shown below.
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