The cascode is a two-stage amplifier that consists of a common-emitter stage feeding into a common-base stage.
This a brief description of how cascode amplifiers function what are the factors that determine the bandwidth of the circuit.
An experiment to determine the value of current gain (Beta) of a transistor using voltmeter. The experiment also includes building a constant current source using bjt and zener diode.
An experiment to determine the value of current gain (Beta) of a transistor using voltmeter. The experiment also includes building a constant current source using bjt and zener diode.
DIFFERENTIAL AMPLIFIER using MOSFET, Modes of operation,
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Frequency-Shift Keying, also known as FSK is a type of digital frequency modulation. It is also often called as binary frequency shift keying or BFSK
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This presentation will discuss the concepts behind FSK
Introduction
Band Pass Amplifiers
Series & Parallel Resonant Circuits & their Bandwidth
Analysis of Single Tuned Amplifiers
Analysis of Double Tuned Amplifiers
Primary & Secondary Tuned Amplifiers with BJT & FET
Merits and de-merits of Tuned Amplifiers
This presentation contains the basics of oscillators, types of oscillators & its mathematical Analysis. Numericals based on each type of oscillator are solved & given for practice.
DIFFERENTIAL AMPLIFIER using MOSFET, Modes of operation,
The MOS differential pair with a common-mode input voltage ,Common mode rejection,gain, advantages and disadvantages.
Frequency-Shift Keying, also known as FSK is a type of digital frequency modulation. It is also often called as binary frequency shift keying or BFSK
Similar to analog FM, it is a constant-amplitude angle modulation.
This presentation will discuss the concepts behind FSK
Introduction
Band Pass Amplifiers
Series & Parallel Resonant Circuits & their Bandwidth
Analysis of Single Tuned Amplifiers
Analysis of Double Tuned Amplifiers
Primary & Secondary Tuned Amplifiers with BJT & FET
Merits and de-merits of Tuned Amplifiers
This presentation contains the basics of oscillators, types of oscillators & its mathematical Analysis. Numericals based on each type of oscillator are solved & given for practice.
EEE 117L Network Analysis Laboratory Lab 1
1
EEE 117L Network Analysis Laboratory
Lab 1 – Voltage/Current Division and Filters
Lab Overview
The objective of Lab 1 is to familiarize students with a variety of basic applications of
passive R, C devices, and also how to measure the performance of these circuits using
both Spice simulations and the Digilent Analog Discovery 2 on the circuits constructed.
Prelab
Before coming to lab, students need to complete the following items for each of the
circuits studied in this lab :
• Any hand calculations needed to determine the values of components used in the
circuits such as resistors and capacitors, or specifications such as pole frequencies.
• A Spice simulation of each circuit to get familiar with how it works, and determine
what to expect when the circuit is built and its performance is measured.
Making connections on a Breadboard
Breadboards are used to easily construct circuits without the need to solder parts on a
printed circuit board. As seen in Figure 0 they have columns of pins that are connected
together internally, so that all the wires inserted in a column are shorted together. Note
that the columns on top and bottom are not connected together. There are also rows of
pins at the top and bottom that are connected together. These rows are intended for use
as the power supplies, and are typically labeled + and – and color coded red and blue for
the positive and negative power supplies. These rows are not connected in the middle.
Figure 0.
EEE 117L Network Analysis Laboratory Lab 1
2
Circuits to be studied
When choosing resistor and capacitor values use standard values available to you,
and keep all resistor values between 100 W and 100 kW.
1. Voltage and Current Dividers
One of the most commonly used circuits is a voltage divider
like the one shown in Figure 1.a. For example, if a signal is
too large to be input to a voltmeter or oscilloscope it can be
attenuated (reduced in size) using voltage division. The DC
voltage that an AC signal like a sine wave varies around can
also be reduced using this circuit.
For example, if all of the resistors in this circuit are the same
value, and the VS input source provides a DC voltage of 4V,
then the voltages in this circuit will be VA = 4V, VB = 3V,
VC = 2V, and VD = 1V. That is, voltage division will cause the voltage at node B to be
¾ of VS , the voltage at node C to be ½ of VS , and the voltage at node D to be ¼ of VS.
If a sine wave with an amplitude of 1V is then added so that VS = 4 + sin(wt) Volts, then
voltage division will cause the new values of VA , VB , VC and VD to be :
VA = 1.00*VS = 1.00*(4 + sin(wt)) = 4 + 1.00*sin(wt) Volts
VB = 0.75*VS = 0.75*(4 + sin(wt)) = 3 + 0.75*sin(wt) Volts
VC = 0.50*VS = 0.50*(4 + sin(wt)) = 2 + 0.50*sin(wt) Volts
VD = 0.25*VS = 0.25*(4 + sin(wt)) = 1 + 0.25*sin(wt) Volts
In this example both the amplitude of the ...
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1. EC 204: ANLOG CIRCUITS LABORATORY
Experiment 4
CE-CB Cascode Amplifier
Sachin Rajoria 08010826
Manzil Zaheer 08010252
Payoj Kissan 08010823
To design CE amplifier and CE-CB case code amplifier and compare their gain and bandwidth.
2. Objective:
To make a single stage CE amplifier and experimentally determine its frequency response.
To modify the CE amplifier into CE-CB case code amplifier and experimentally determine its
frequency response.
To compare the gain and bandwidth of CE amplifier with that of CE-CB case code amplifier and
justify the result.
Instruments/Materials Required:
1. NPN Transistor: 2N2222A x2
2. Capacitors:
I. 10 µF x3
II. 100 µF x1
3. Resistors:
a. 1 kΩ x5
b. 3.3 kΩ x1
c. 10 kΩ x1
d. 22 kΩ x2
e. 100 kΩ x1
f. 150 kΩ x2
4. Breadboard x1
5. Function generator x1
6. DC Power Supply: 15V x1
Theory:
3. Bandwidth=𝐹𝐹𝐻𝐻 − 𝐹𝐹𝐿𝐿
If 𝐹𝐹𝐻𝐻 ≫ 𝐹𝐹𝐿𝐿 , then
∴ Bandwidth≈ 𝐹𝐹𝐻𝐻
The capacitors in the circuit determine the frequency response i.e. lower and higher cut-off frequencies.
General expression of gain
As =
𝑎𝑎 𝑚𝑚 (𝑠𝑠 + 𝑤𝑤𝑧𝑧1)(𝑠𝑠 + 𝑤𝑤𝑧𝑧2) … … … … … … . (𝑠𝑠 + 𝑤𝑤𝑧𝑧𝑧𝑧 )
�𝑠𝑠 + 𝑤𝑤𝑝𝑝1��𝑠𝑠 + 𝑤𝑤𝑝𝑝2� … … … … . �𝑠𝑠 + 𝑤𝑤𝑝𝑝𝑝𝑝 �
Dominant pole approximation
wL ≈ wp1 (two octave or four time higher)
: if wpi ≫ all other poles and zero frequencies,wp1 is the dominant pole
frequency and
In the case of no dominant pole wL = �(𝑤𝑤𝑝𝑝1
2
+ 𝑤𝑤𝑝𝑝2
2
… − 2𝑤𝑤𝑧𝑧1
2
− 2𝑤𝑤𝑧𝑧2
2
… )
High frequency response
Gain
As =
𝑎𝑎 𝑚𝑚 �1 +
𝑠𝑠
𝑤𝑤 𝑧𝑧1
� �1 +
𝑠𝑠
𝑤𝑤 𝑧𝑧2
� … . . �1 +
𝑠𝑠
𝑤𝑤 𝑧𝑧𝑧𝑧
�
�1 +
𝑠𝑠
𝑤𝑤 𝑝𝑝1
� �1 +
𝑠𝑠
𝑤𝑤 𝑝𝑝2
� … . . �1 +
𝑠𝑠
𝑤𝑤 𝑝𝑝𝑝𝑝
�
:
If wp1 ≪ all other poles and zero frequencies then,
wH ≈ wp1
Else
wH =
1
�
1
wp1
2 +
1
wp2
2 … − 2 �
1
wz1
2 +
1
wz2
2 + ⋯ +
1
wzn
2 �
4. CE Amplifier
…
Calculation of lower cut-off frequency of CE amplifier
Cut-off frequency of capacitor at input
:
∴ 𝐹𝐹𝐶𝐶 =
1
2𝜋𝜋𝑅𝑅𝑒𝑒𝑒𝑒 𝐶𝐶𝑒𝑒𝑒𝑒
Where: Req = �R6 + R2�|R1|�β(R3)�
= (1k+22k||100k||170 (1k))
=16.30kΩ
Ceq =10µF
∴ 𝐹𝐹𝐶𝐶 = 0.9764𝐻𝐻𝐻𝐻
β
5. Cut-off frequency of emitter capacitance
∴ 𝐹𝐹𝐶𝐶 =
1
2𝜋𝜋𝑅𝑅𝑒𝑒𝑒𝑒 𝐶𝐶𝑒𝑒𝑒𝑒
Where: Req = R1||R3
R1 = 1kΩ
R3 = re +
𝑅𝑅6�|𝑅𝑅2|�𝑅𝑅1
𝛽𝛽
re =
VT
IE
=
26𝑚𝑚𝑚𝑚
1.87𝑚𝑚𝑚𝑚
= 13.90Ω
Req = 13.70 Ω
∴ 𝐹𝐹𝐶𝐶 = 116.17𝐻𝐻𝐻𝐻
Cut-off frequency of out-put capacitance
∴ 𝐹𝐹𝐶𝐶 =
1
2𝜋𝜋𝑅𝑅𝑒𝑒𝑒𝑒 𝐶𝐶𝑒𝑒𝑒𝑒
Where: Req = 3.3𝑘𝑘 + 10𝑘𝑘
=13.3kΩ
Ceq = 10µF
∴ 𝐹𝐹𝐶𝐶 = 1.19𝐻𝐻𝐻𝐻
∴The lower cut-off frequency of CE amplifier is=116.17Hz
6. Calculation of higher cut-off frequency of CE amplifier
Let A is the gain of CE amplifier
𝐴𝐴 = �−
𝑅𝑅𝐶𝐶||𝑅𝑅𝐿𝐿
𝑟𝑟𝑒𝑒
�
:
Where:
RL = 10kΩ
RC = 3.3kΩ
re = 13.90Ω
Gain 𝐴𝐴 = 178.50
Ceq = Cin = Cπ + Cμ(1 + A)
From data sheet Cπ = 25pF, Cμ = 8pF
Cin = 1559.89pF
Rin = �rx + RS�|R2|�R3�||βre
= 676.04Ω
Fin,H = 150.922kHz
Fout ,H =
1
2π(Rc||RL)(Cμ �
1
A
+ 1�)
=8.62MHz
∴The higher frequency cut-off of the CE amplifier=150.922kHz
7. CE-CB case-code amplifier
Calculation of lower cut-off frequency of CE –CB amplifier
Calculation of frequency due to emitter resistance
:
Rnet = R1||R3
= 1k|| �13.90Ω +
�22k�|25k|�1k�
170
�
= 18.953Ω
FCE = 83.98Hz
8. Calculation of frequency due to out-put resistance
Fc,out =
1
2π(3.3k + 10k)(10μF)
=1.19Hz
Calculation of frequency due to input capacitance
Rnet = R6 + �R7�|R2|�βR3�
=1k+ (22k||25k||130(1k))
=11.73kΩ
FC=1.35Hz
Calculation of frequency due to CB
𝐹𝐹𝐶𝐶𝐶𝐶 =
1
2𝜋𝜋(25𝑘𝑘||75𝑘𝑘)(10𝜇𝜇𝜇𝜇)
=0.849Hz
Theoretical justification
The lower cut-off frequency of both CE and CE-CB case code amplifier are almost equal.
:-
9. CE amplifier (high frequency)
Because the gain of the CE amplifier is very high, the Miller capacitance transferred to the input side i.e.
Cµ(A + 1) because very large and as the result the higher cut-off frequency which is determined by it
decreases.
FH =
1
2π �Cπ + Cμ(A + 1)� Req
:
Gain A = ()
∴ FH is decreased considerably
The Miller capacitance at the output side does not play a role in determining FH because Cµ �
1
A
+ 1� is
approximately equal to Cμ and therefore the frequency determined by it, is higher compared to that at
the input
∴ The frequency determined by the capacitance at the input side is the dominant frequency and
determines the higher cut-off frequencies.
CE-CB case code amplifiers:-
CE stage:-
The difference between the CE stage of CE-CB case code and CE amplifier is the gain.
The gain of the CE stage in the CE-CB case code is given by this approximation, Gain is =
re2
re1
≈ 1
The Miller capacitance at the input in case of CE-CB case code is much lower than that of CE
amplifier. The frequency due to the Miller capacitance at input in case of CE-CB case code is higher as
compare to the CE amplifier.
10. 𝐹𝐹ℎ1 =
1
2𝜋𝜋(𝐶𝐶𝜋𝜋+ 𝐶𝐶𝜇𝜇 ( ))𝑅𝑅𝑒𝑒𝑒𝑒
>
1
2𝜋𝜋(𝐶𝐶𝜋𝜋+ 𝐶𝐶𝜇𝜇 ( ))𝑅𝑅𝑒𝑒𝑒𝑒
Bandwidth of the CE-CB amplifier is higher than that of CE amplifier.
CB stage:-
The frequency response due to Cπ is much smaller as compared to Cμ.
The frequency response due toCμ,
Fcb =
1
2πCμ(Rc ||RL )
This frequency is comparable to frequency determined by the input side of CE stage in CE-CB case code.
∴ FH =
1
�
1
Fμ
+
1
Fh1
Thus, the net high frequency cut-off calculated is higher than the case of CE amplifier.
15. CE-CB case code
The midband gain, Av midband = 104
Av midband
√2
= 73.5
:-
From the observation table,
FH ≈ 500 kHz.
Bandwidth ≈ 500 kHz.
Result:
The bandwidth of CE-CB case code amplifier is higher than that of a CE amplifier.