Common-Base amplifier using npn transistor:
In this type of amplifier, the input signal is applied between emitter and base terminals and the output signal is obtained across the collector and base terminals through the load resistance
(RL). The base is common to both the input and output terminals.
The amplifier circuit using npn transistor is as shown:
The input a.c signal is applied across the emitter and base circuit which is forward biased by a battery of emf VEB. The output signal is taken across load resistance (RL) connected across collector-Base circuit, which is reverse biased by a battery of emf VCB.
The emitter current (IC) is given by
Ie=Ib+Ic ...(i)
Ib and Ic are base and collector current respectively.
If no current flows through the load resistance, then the voltage across output circuit is the emf of the battery i.e. VCB.
If current Ic flows through RL, then voltage across output circuit is: Vo=VCB+IcRL ...(ii)
Now, when the applied input signal increases on positive half cycle, the forward bias between emitter-base junction decreases i.e. becomes less negative. As a result, emitter current decreases and hence according to (i), collector current IC also decreases. Thus, potential drop across RL(=ICRL) decreases.
Hence, from equation (ii), we find that Vo decreases.
When applied input decreases on negative half cycle, forward bias between emitter-base junction increases. Due to increased forward bias, emitter current (Ie) increases and hence according to (i); IC also increases.
Thus potential drop across RL(ICRL) also increases. Therefore, from (ii) we find that Vo decreases.
Thus, in common Base amplifier, collector voltage increases with increasing input signal and decreases with decreasing input signal.
This shows that input and amplified output signals are in phase.
Given, RL=600kΩ
Ri = Input resistance = 150pΩ
Current amplification = 0.90
Voltage amplification = ?
Voltage Amplification= Current amplification x Resistance gain
⇒=0.90×RLRi
⇒=0.90×150pΩ600kΩ
⇒=90100×14×10−12103
⇒=22.5×10−17