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Common Base Amplifier

1673_common base amplifier.png 
The common base amplifier circuit is given  in the figure 1.  The  VEE source forward biases emitter diode and VCC  source reverse biased collector diode. The AC source vin is connected to  emitter through a coupling capacitor such that it blocks DC. This ac voltage produces small variation in currents and voltages. The load resistance RL is connected to collector through coupling capacitor also so the variation in collector base voltage will be observed across RL.

The DC equivalent circuit can be obtained by  reducing  all the AC  sources  to  zero Figure 1 and  opening  all the capacitors. The dc collector current is same as IE  and VCB can be given by

VCB = VCC - IC RC.

The current and voltage fix Q point. The AC equivalent circuit can be obtained by reducing all the DC sources to zero and shorting all the coupling capacitors. r'e represents AC resistance of the diode as shown in the figure 2.

1659_common base amplifier1.png

Figure 2

Figure 3, shows diode curve relating IE  and VBE. In absence of the AC signal, the transistor operates at Q point. When the AC signal is applied, the emitter current and voltage also change. If signal is small, the operating point swings sinusoidally about Q point.

212_common base amplifier2.png

Fig .3

If AC signal is small, the points A and B are near to Q, and arc A B can be approximated by a straight line and diode appears to be the resistance which is given by

1051_common base amplifier3.png

If input signal is small, input voltage and current will be sinusoidal in nature but if the input voltage is large then the current will no longer be sinusoidal due to the non linearity of diode curve. The emitter current is elongated on positive half cycle and compressed on the negative half cycle. Hence output will also be distorted.

r'e  is the ratio of ΔVBE and Δ IE and its value depends upon location of the Q. Higher up the Q point small will be value of r' e because same change in VBE produces the large change in IE. The slope of curve at Q decides the value of r'e. From the calculation it can be proved that

r'e = 25mV / IE

Proof-

Generally the current through a diode can be given by

529_proof of equation.png

Where q is the charge on electron, V is drop across diode, T is temperature and K is a constant.

On differentiating with respect to V, we get,

  61_proof of equation4.png 
The value of (q / KT) at temperature 25°C is approximately 40. Therefore,  

617_proof of equation1.png

or,     

650_proof of equation2.png

1488_proof of equation3.png

To a close approximation small changes in the collector current equal the small changes in emitter current. In AC equivalent circuit, the current =iC' is shown upward as if =ie' increases, then =iC' also increases in same direction.

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