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20IM10045 - Sahil Agrawal - Exp 4

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Name: Sahil Agrawal

Roll Number: 20IM10045

Aim of the Experiment

To investigate the operation of a common-emitter NPN transistor amplifier.

Tools Used

S. No. Apparatus Range Type Quantity

1 Resistor - 1
i) 100Ω -1000Ω
2
ii)100Ω - 4000Ω
iii)100Ω-47kΩ 1
iv)100Ω-15kΩ 1
2 Voltage Source 50Hz-50MHz i)AC 1
ii)DC 1
3 Capacitor 1μF-10μF - 3

4 BJT - NPN 1

Background Knowledge-

The common emitter configuration is widely used as a basic amplifier as it has both voltage and
current amplification.
Resistors RB1 and RB2 form a voltage divider across the base of the transistor. The function of
this network is to provide necessary bias conditions and ensure that the emitter-base junction is
operating in the proper region.
In order to operate a transistor as an amplifier, biasing is done in such a way that the operating
point is in the active region. For an amplifier the Q-point is placed so that the load line is bisected.
Therefore, in practical design VCE is always set to VCC/2. This will confirm that the Q-point
always swings within the active region. This limitation can be explained by maximum signal
handling capacity. For the maximum input signal, output is produced without any distortion and
clipping.

Input Capacitor (C1)


The capacitor C1 is used to couple the signal to the base terminal of the BJT. If it is not there, the
signal source resistance, Rs will come across R2 and hence, it will change the bias. C1 allows
only the AC signal to flow but isolates the signal source from R2

Emitter Bypass Capacitor (CE)


An Emitter bypass capacitor CE is used parallel with RE to provide a low reactance path to the
amplified AC signal. If it is not used, then the amplified AC signal following through RE will cause a
voltage drop across it, thereby dropping the output voltage.

Coupling Capacitor (C2)


The coupling capacitor C2 couples one stage of amplification to the next stage. This technique
used to isolate the DC bias settings of the two coupled circuits.

CE Amplifier Frequency Response


The voltage gain of a CE amplifier varies with signal frequency. It is because reactances of the
capacitors in the circuit changes with signal frequency and hence affects the output voltage. The
curve drawn between voltage gain and the signal frequency of an amplifier is known as frequency
response. Below figure shows the frequency response of a typical CE amplifier.

Frequency Response of Common Emitter Amplifier

The midband gain is obtained by short circuiting all the external capacitors and open circuiting
the internal capacitors. Figure 2 shows the equivalent for calculating the midband gain.
The high frequency equivalent circuit of the common-emitter amplifier is shown in Figure 3.

Circuit Diagrams:
Serial Frequency(Hz) Magnitude(dB)
No.

1 80 4.77432

2 96 6.43712

3 183 12.1336

4 318 16.92652

5 727 23.917

6 1386 28.8692

7 2197 31.7644

8 4186 34.393

9 8746 35.606

10 20036 35.9562

11 26413 35.9928

12 38179 36.0186

13 79766 36.0352

14 105153 36.0358

15 138618 36.034

16 200364 36.0272

17 264131 36.0166

18 381786 35.9884

19 727478 35.8484

20 1051530 35.646

21 2003640 34.7474

22 4590080 31.5338

23 9590030 26.5178
24 45900800 13.4081

Source Resistance (RS): 100 Ω


Collector Resistance (RC): 500Ω
Emitter Resistance (RE): 1000 Ω
Load Resistance (RL): 2000 Ω
Base Resistance (RB1): 5000 Ω
Base Resistance (RB2): 5000 Ω
Coupling Capacitor (CC1): 10 μF
Coupling Capacitor (CC2): 10 μF
Bypass Capacitance (CE): 10 μF

Graph:

Midband gain = -63.41 Hz


Low frequency cut-off = 17882.65323 Hz
High frequency cut-off= 2.13515e+7 Hz
1) Frequency Response

a) Load Resistance is Connected

Circuit Diagram of CE Amplifier for Frequency Response

CE Frequency Response

Low frequency cut-off = 64.874Hz


High frequency cut-off= 10.841 MHz
b) Load Resistance is not connected

Circuit Diagram of CE Amplifier for Frequency Response

CE Frequency Response

Low frequency cut-off = 90.331Hz


High frequency cut-off= 11.415 MHz
2) Signal Handling Capacity

a) Load Resistance is connected

CE Amplifier Circuit for Signal Handling Capacity

CE Amplifier V(out)/V(in) in Time Domain

Peak Voltage = 17.5 mV


Vin = 1mV
Gain =V(out)/V(in) = 17.5/1 = 17.5
Vsm = 300 mV
b) Load Resistance isn’t connected

CE Amplifier Circuit for Signal Handling Capacity

CE Amplifier V(out)/V(in) in Time Domain

Peak Voltage = 18.5 mV


Vin = 1mV
Gain = V(out)/V(in) = 18.5/1 = 18.5
Vsm = 300 mV
3) DC Analysis

Circuit Diagram for DC Analysis

Model of BJT being used - 2N3904

V(b)=1.08202 V
V(c) = 7.49125 V
V(e) = 0.438987 V

Ic = 0.663051mA
Ie = 0.665131 mA
Calculations:
Discussions:
At low frequencies (< FL) the reactance of coupling capacitor C2 is relatively high and
hence very small part of the signal will pass from amplifier stage to the load.
Moreover, CE cannot shunt the RE effectively because of its large reactance at low
frequencies. These two factors cause a drop off of voltage gain at low frequencies.
At high frequencies (> FH) the reactance of coupling capacitor C2 is very small and it
behaves as a short circuit. This increases the loading effect of the amplifier stage and
serves to reduce the voltage gain.
Moreover, at high frequencies, the capacitive reactance of base-emitter junction is low
which increases the base current. This frequency reduces the current amplification
factor β. Due to these two reasons, the voltage gain drops off at high frequency.
At mid frequencies (FL to FH) the voltage gain of the amplifier is constant. The effect of
the coupling capacitor C2 in this frequency range is such as to maintain a constant
voltage gain. Thus, as the frequency increases in this range, the reactance of CC
decreases, which tends to increase the gain. However, we observe that the voltage gain
drops off at low (< FL) and high (> FH) frequencies, whereas it is constant over the mid-
frequency range (FL to FH).

Conclusion:
Conclusion from Above Curves :
a) Frequency Response : The voltage gain drops off at low (< FL) and high
(> FH) frequencies, whereas it is constant over the mid-frequency range
(FL to FH). Also the gain in case of no load connected is more compared
to when load is connected.
b) Signal Handling Capacity : The output voltage is higher than the input
voltage whether load is connected or not, thus input is amplified in
both the cases. However on connecting the load resistance, the peak
voltage decreases. We also observe a shift of 1800
c) DC Analysis : We see the stabilization of the Q-point.Vcc is greater
than Vce, thus the amplifier is biased in the active region.
In Common Emitter Amplifier, Input is applied to B-E Junction and Output is taken from E-C
Terminal, here the emitter terminal is common for both input and output.
It is a widely used amplifier circuit because it provides good current gain and good voltage
gain and it is also known as an inverting amplifier because it gives 180° phase shift from
input to output. It is widely used in audio amplification and signal amplification circuits. The
current gain and voltage are moderate. However, in the CE amplifier, there is high thermal
instability.

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