DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING IC APPLICATIONS LABORATORY 1 1. Study of OP AMPs - IC 741, IC 555, IC 565, IC 566, IC 1496-functioning, parameters and specifications IC 741 General Description The IC 741 is a high performance monolithic operational amplifier constructed using the planer epitaxial process. High common mode voltage range and absence of latch-up tendencies make the IC 741 ideal for use as voltage follower. The high gain and wide range of operating voltage provide superior performance in integrator, summing amplifier and general feed back applications. Internal Block Diagram of Op-Amp Fig.1: Block diagram of op-amp Pin Configuration Fig.2: Pin diagram of IC741
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DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING
IC APPLICATIONS LABORATORY
1
1. Study of OP AMPs - IC 741, IC 555, IC 565, IC 566,
IC 1496-functioning, parameters and specifications
IC 741
General Description
The IC 741 is a high performance monolithic operational amplifier constructed
using the planer epitaxial process. High common mode voltage range and absence
of latch-up tendencies make the IC 741 ideal for use as voltage follower. The high
gain and wide range of operating voltage provide superior performance in integrator,
summing amplifier and general feed back applications.
Internal Block Diagram of Op-Amp
Fig.1: Block diagram of op-amp
Pin Configuration
Fig.2: Pin diagram of IC741
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Features
1. No frequency compensation required.
2. Short circuit protection
3. Offset voltage null capability
4. Large common mode and differential voltage ranges
5. Low power consumption
6. No latch-up
Specifications
1. Voltage gain A = α typically 2,00,000
2. I/P resistance RL = α Ω, practically 2MΩ
3. O/P resistance R =0, practically 75Ω
4. Bandwidth = α Hz. It can be operated at any frequency
5. Common mode rejection ratio = α
(Ability of op amp to reject noise voltage)
6. Slew rate + α V/µsec
(Rate of change of O/P voltage)
7. When V1 = V2, VD=0
8. Input offset voltage (Rs ≤ 10KΩ) max 6 mv
9. Input offset current = max 200nA
10. Input bias current : 500nA
11. Input capacitance : typical value 1.4pF
12. Offset voltage adjustment range : ± 15mV
13. Input voltage range : ± 13V
14. Supply voltage rejection ratio : 150 µV/V
15. Output voltage swing: + 13V and – 13V for RL > 2KΩ
16. Output short-circuit current: 25mA
17. supply current: 28mA
18. Power consumption: 85mW
19. Transient response: rise time= 0.3 µs
Overshoot= 5%
Applications
1. AC and DC amplifiers
2. Active filters
3. Oscillators
4. Comparators
5. Regulators
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IC 555
General Description
The operation of SE/NE 555 timer directly depends on its internal function.
The three equal resistors R1, R2, R3 serve as internal voltage divider for the source
voltage. Thus one-third of the source voltage VCC appears across each resistor.
Comparator is basically an Op amp which changes state when one of its
inputs exceeds the reference voltage. The reference voltage for the lower
comparator is +1/3 VCC. If a trigger pulse applied at the negative input of this
comparator drops below +1/3 VCC, it causes a change in state. The upper comparator
is referenced at voltage +2/3 VCC. The output of each comparator is fed to the input
terminals of a flip flop.
The flip-flop used in the SE/NE 555 timer IC is a bistable multivibrator. This
flip flop changes states according to the voltage value of its input. Thus if the voltage
at the threshold terminal rises above +2/3 VCC, it causes upper comparator to cause
flip-flop to change its states. On the other hand, if the trigger voltage falls below +1/3
VCC, it causes lower comparator to change its states. Thus the output of the flip flop
is controlled by the voltages of the two comparators. A change in state occurs when
the threshold voltage rises above +2/3 VCC or when the trigger voltage drops below
+1/3 Vcc.
The output of the flip-flop is used to drive the discharge transistor and the
output stage. A high or positive flip-flop output turns on both the discharge transistor
and the output stage. The discharge transistor becomes conductive and behaves as
a low resistance short circuit to ground. The output stage behaves similarly. When
the flip-flop output assumes the low or zero states reverse action takes place i.e., the
discharge transistor behaves as an open circuit or positive VCC state. Thus the
operational state of the discharge transistor and the output stage depends on the
voltage applied to the threshold and the trigger input terminals.
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Block Diagram of IC 555
Fig.3: Block diagram of IC 555
Pin Configuration
Fig.4: Pin diagram of IC555
Function of Various Pins
Pin (1) of 555 is the ground terminal; all the voltages are measured with respect to
this pin.
Pin (2) of 555 is the trigger terminal, if the voltage at this terminal is held greater than
one-third of VCC, the output remains low. A negative going pulse from Vcc to less than
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Vec/3 triggers the output goes to High. The amplitude of the pulse should be able to
make the comparator (inside the IC) change its state. However the width of the
negative going pulse must not be greater than the width of the expected output pulse.
Pin (3) is the output terminal of IC 555. There are 2 possible output states. In the
low output state, the output resistance appearing at pin (3) is very low (approximately
10 Ω). As a result the output current will goes to zero , if the load is connected from
Pin (3) to ground , sink a current I Sink (depending upon load) if the load is connected
from Pin (3) to ground, and sinks zero current if the load is connected between +VCC
and Pin (3).
Pin (4) is the Reset terminal. When unused it is connected to +Vcc. Whenever the
potential of Pin (4) is drives below 0.4V, the output is immediately forced to low state.
The reset terminal enables the timer over-ride command signals at Pin (2) of the IC.
Pin (5) is the Control Voltage terminal. This can be used to alter the reference levels
at which the time comparators change state. A resistor connected from Pin (5) to
ground can do the job. Normally 0.01µF capacitor is connected from Pin (5) to
ground. This capacitor bypasses supply noise and does not allow it affect the
threshold voltages.
Pin (6) is the threshold terminal. In both astable as well as monostable modes, a
capacitor is connected from Pin (6) to ground. Pin (6) monitors the voltage across
the capacitor when it charges from the supply and forces the already high O/p to Low
when the capacitor reaches +2/3 VCC.
Pin (7) is the discharge terminal. It presents an almost open circuit when the output
is high and allows the capacitor charge from the supply through an external resistor
and presents an almost short circuit when the output is low.
Pin (8) is the +Vcc terminal. 555 can operate at any supply voltage from +3 to +18V.
Features
1. The load can be connected to o/p in two ways i.e. between pin 3 & ground 1 or
between pin 3 & VCC (supply)
2. 555 can be reset by applying negative pulse, otherwise reset can be connected
to +Vcc to avoid false triggering.
3. An external voltage effects threshold and trigger voltages.
4. Timing from micro seconds through hours.
5. Monostable and bistable operation
6. Adjustable duty cycle
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7. Output compatible with CMOS, DTL, TTL
8. High current output sink or source 200mA
9. High temperature stability
10. Trigger and reset inputs are logic compatible.
Specifications
1. Operating temperature : SE 555-- -55oC to 125oC
NE 555-- 0o to 70oC
2. Supply voltage : +5V to +18V
3. Timing : µSec to Hours
4. Sink current : 200mA
5. Temperature stability : 50 PPM/oC change in temp or 0-005% /oC.
Applications
1. Monostable and Astable Multivibrators
2. dc-ac converters
3. Digital logic probes
4. Waveform generators
5. Analog frequency meters
6. Tachometers
7. Temperature measurement and control
8. Infrared transmitters
9. Regulator & Taxi gas alarms etc.
IC 565
General Description
The Signetics SE/NE 560 series is monolithic phase locked loops. The SE/NE 560,
561, 562, 564, 565, & 567 differ mainly in operating frequency range, power supply
requirements and frequency and bandwidth adjustment ranges. The device is
available as 14 Pin DIP package and as 10-pin metal can package. Phase
comparator or phase detector compare the frequency of input signal fs with frequency
of VCO output fo and it generates a signal which is function of difference between the
phase of input signal and phase of feedback signal which is basically a d.c voltage
mixed with high frequency noise. LPF remove high frequency noise voltage. Output
is error voltage. If control voltage of VCO is 0, then frequency is center frequency (fo)
and mode is free running mode. Application of control voltage shifts the output
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frequency of VCO from fo to f. On application of error voltage, difference between fs
& f tends to decrease and VCO is said to be locked. While in locked condition, the
PLL tracks the changes of frequency of input signal.
Block Diagram of IC 565
Fig.5: Block Diagram of IC 565
Pin Configuration
Fig.6: Pin diagram of IC 565
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Specifications
1. Operating frequency range : 0.001 Hz to 500 KHz
2. Operating voltage range : ±6 to ±12V
3. Inputs level required for tracking : 10mV rms minimum to 3v (p-p)
max.
4. Input impedance : 10 KΩ typically
5. Output sink current : 1mA typically
6. Drift in VCO center frequency : 300 PPM/oC typically
(fout) with temperature
7. Drif in VCO centre frequency with : 1.5%/V maximum
supply voltage
8. Triangle wave amplitude : typically 2.4 VPP at ± 6V
9. Square wave amplitude : typically 5.4 VPP at ± 6V
10. Output source current : 10mA typically
11. Bandwidth adjustment range : <±1 to >± 60%
Center frequency fout = 1.2/4R1C1 Hz
= free running frequency
FL = ± 8 fout/V Hz
V = (+V) – (-V)
fc = ± ] 2/1
3210)6.3(2
Π xCx
f L
Applications
1. Frequency multiplier
2. Frequency shift keying (FSK) demodulator
3. FM detector
IC 566
General Description
The NE/SE 566 Function Generator is a voltage controlled oscillator of
exceptional linearity with buffered square wave and triangle wave outputs. The
frequency of oscillation is determined by an external resistor and capacitor and the
voltage applied to the control terminal. The oscillator can be programmed over a ten
to one frequency range by proper selection of an external resistance and modulated
over a ten to one range by the control voltage with exceptional linearity.
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Block Diagram of IC566
Fig.7: Block diagram of IC566
Pin diagram
Fig.8 : Pin diagram of IC566
Specifications
Maximum operating Voltage --- 26V
Input voltage --- 3V (P-P)
Storage Temperature --- -65oC to + 150oC
Operating temperature --- 0oC to +70oC for NE 566
-55oC to +125oC for SE 566
Power dissipation --- 300mv
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Applications
1. Tone generators.
2. Frequency shift keying
3. FM Modulators
4. clock generators
5. signal generators
6. Function generator
IC 1496
General Description
IC balanced mixers are widely used in receiver IC’s. The IC versions are
usually described as balanced modulators. Typical example of balanced IC
modulator is MC1496. The circuit consists of a standard differential amplifier (formed
by Q5 _ Q6 combination) driving a quad differential amplifier composed of transistor
Q1 – Q4. The modulating signal is applied to the standard differential amplifier
(between terminals 1 and 4). The standard differential amplifier acts as a voltage to
current converter. It produces a current proportional to the modulating signal. Q7 and
Q8 are constant current sources for the differential amplifier Q5 – Q6. The lower
differential amplifier has its emitters connected to the package pins ( 2 & 3) so that an
external emitter resistance may be used. Also external load resistors are employed
at the device output (6 and 12 pins).The output collectors are cross-coupled so that
full wave balanced multiplication takes place. As a result, the output voltage is a
constant times the product of the two input signals.
Schematic of IC1496
Fig.9: Pin diagram of IC1496
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Pin Configuration
Fig.10 : Pin diagram of IC1496
Applications of MC 1496
• Balanced modulator
• AM Modulator
• Product Modulator
• AM Detector
• Mixer
• Frequency Doublers.
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2. OP AMP Applications – Adder, Subtractor,
Comparator Circuits
Aim: To design Adder, Subtractor and Comparator circuits by using operational
amplifier.
Apparatus required
S.No Equipment/Component name Specifications/Value Quantity
1 IC 741 Refer page no 2 1
2 Resistor 1kΩ 4
3 Diode 0A79 2
4 Regulated Power supply (0 – 30V),1A 2
5 Function Generator (.1 – 1MHz), 20V p-p 1
6 Cathode Ray Oscilloscope (0 – 20MHz) 1
7 Multimeter 3 ½
digit display 1
Theory
Adder: A two input summing amplifier may be constructed using non-inverting
mode or inverting mode. The gain of this summing amplifier is 1 as all the resistors
are equal in value; any scaling factor can be obtained by selecting proper external
resistors.
Subtractor: A basic differential amplifier can be used as a subtractor as shown in
fig.3. In this circuit all external resistors are equal in value. Hence the gain of
amplifier is equal to one. The output voltage Vo is equal to the difference voltage
between the non-inverting terminal and the inverting terminal; hence the circuit is
called a subtractor.
Comparator: The circuit diagram shows an op-amp used as a comparator. A
fixed reference voltage Vref is applied to the one terminal and the varying signal
voltage Vin is applied to the other terminal. Depending upon the application of Vin to
the terminal this can be non inverting or inverting, if input Vin is connected to the non
inverting terminal of the op-amp then it is called as non- inverting comparator as vice
versa. Depending upon the levels of Vin and Vref, the circuit produces output +Vsat or
-Vsat
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Circuit Diagrams
Adder:
Fig. 1: Non- inverting Adder
Fig. 2: Inverting Adder
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Subtractor
Fig. 3: Subtractor
Comparator
Fig. 4: Non-inverting Comparator
Fig. 5: Inverting Comparator
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Designing & Model Calculations
Adder
Non-inverting
Vo = (V1 + V2)
If V1 = 2.5V and V2 = 2.5V, then
Vo = (2.5+2.5) = 5V.
Inverting
Vo = - (V1 + V2)
If V1 = 2.5V and V2 = 2.5V, then
Vo = - (2.5+2.5) = -5V.
Subtractor
Vo = V2 – V1
If V1=2.5 and V2 = 3.3, then
Vo = 3.3 – 2.5 = 0.8V
Comparator
Non-inverting
If Vin < Vref, Vo = -Vsat ≅ - VEE
Vin > Vref, Vo = +Vsat = +VCC
Inverting
If Vin < Vref, Vo = +Vsat ≅ +VCC
Vin > Vref, Vo = -Vsat = - VEE
Procedures
Adder
• Connect the circuit as per the diagram shown in Fig.1 and Fig.2.
• Apply the supply voltages of +15V to pin7 and pin4 of IC741 respectively.
• Apply the inputs V1 and V2 as shown in Fig.1 and Fig.2.
• Apply two different signals (DC/AC ) to the inputs
• Vary the input voltages and note down the corresponding output at pin 6 of the IC
741 adder circuit.
• Notice that the output is equal to the sum of the two inputs.
Subtractor
1. Connect the circuit as per the diagram shown in Fig.3.
2. Apply the supply voltages of +15V to pin7 and pin4 of IC741 respectively.
3 Apply the inputs V1 and V2 as shown in Fig.3.
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4. Apply two different signals (DC/AC) to the inputs
5. Vary the input voltages and note down the corresponding output at pin 6 of the IC
741 subtractor circuit.
7. Notice that the output is equal to the difference of the two inputs.
Comparator
1. A fixed reference voltage Vref and varying voltage Vin is applied as shown in Fig.3
and Fig.4.
2. Vary the input voltage above and below the Vref and note down the output at pin
6 of 741 IC.
3. Observe that,
when Vin is less than Vref,
Output voltage is Non-inverting Inverting
-Vsat ( ≅ - VEE) +Vsat (≅+VCC)
when Vin is greater than Vref,
Output voltage is Non-inverting Inverting
+Vsat (≅+VCC) -Vsat ( ≅ - VEE)
Observations
Adder
V1(V)
V2(V)
Inverting adder
Vo(V)
Non-Inverting
adder Vo(V)
Subtractor
V1(V) V2(V) Vo(V)
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Comparator
Vin(V)
Vref(V)
Non-Inverting
comparator
Vo(V)
Inverting
comparator
Vo(V)
Precautions
Check the connections before giving the power supply.
Readings should be taken carefully.
Results
Inferences
Questions
1. What is the saturation voltage of 741 in terms of VCC?
2. What is the maximum voltage that can be given at the inputs?
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3. Integrator and Differentiator Circuits using IC 741
Aim: To design and verify the operation of an integrator and differentiator for a
given input.
Apparatus required
S.No Equipment/Component name Specifications/Value Quantity
1 741 IC Refer page no. 2 1
2 Capacitors 0.1µf, 0.01µf Each one
3 Resistors 159Ω, 1.5kΩ Each one
4 Regulated Power supply (0 – 30)V,1A 1
5 Function generator (1Hz – 1MHz) 1
6 Cathode Ray Oscilloscope (0 – 20MHz) 1
Theory
Integrator
In an integrator circuit, the output voltage is integral of the input signal. The
output voltage of an integrator is given by Vo = -1/R1Cf Vidt
t
o
∫
At low frequencies the gain becomes infinite, so the capacitor is fully charged and
behaves like an open circuit. The gain of an integrator at low frequency can be
limited by connecting a resistor in shunt with capacitor.
Differentiator
In the differentiator circuit the output voltage is the differentiation of the input
voltage. The output voltage of a differentiator is given by Vo = -RfC1 dt
dVi .The input
impedance of this circuit decreases with increase in frequency, thereby making the
circuit sensitive to high frequency noise and the circuit may become unstable. Hence
an input resistor is connected in series with the capacitor and a capacitor is
connected in parallel with the feedback resistor.
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Circuit Diagrams
Fig. 1: Integrator
Fig. 2: Differentiator
Design equations
Integrator
Choose T = 2πR1Cf
Where T= Time period of the input signal
Assume Cf and find R1
Select Rf = 10R1
Vo (p-p) = dtVCR
ppi
T
of
)(
2/
1
1−∫
−
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Differentiator
Select given frequency fa = 1/(2πRfC1), Assume C1 and find Rf
Select fb = 10 fa = 1/2πR1C1 and find R1
From R1C1 = RfCf, find Cf
Model Calculations
Integrator
For T= 1 msec
fa= 1/T = 1 KHz
fa = 1 KHz = 1/(2πR1Cf)
Assuming Cf= 0.1µf, Rf is found from R1=1/(2πfaCf)
R1=1.59 KΩ
Rf = 10 R1
Rf= 15.9kΩ
Differentiator
For T = 1 msec
f= 1/T = 1 KHz
fa = 1 KHz = 1/(2πRfC1)
Assuming C1= 0.1µf, Rf is found from Rf=1/(2πfaC1)
Rf=1.59 KΩ
fb = 10 fa = 1/2πR1C1
for C1= 0.1µf; R1 =159Ω
Procedures
Integrator
1. Connect the circuit as per the diagram shown in Fig.1
2. Apply a square wave/sine input of 4V(p-p) at 1KHz
3. Observe the output at pin 6.
4. Draw input and output waveforms as shown in Fig.3.
Differentiator
1. Connect the circuit as per the diagram shown in Fig. 2
2. Apply a square wave/sine input of 4V(p-p) at 1KHz
3. Observe the output at pin 6
4. Draw the input and output waveforms as shown in Fig.4
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Wave Forms
Integrator
Fig. 3: Input and output waves forms of integrator
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Differentiator
Fig. 4 : Input and output waveforms of Differentiator
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Observations
Integrator
Input –Square wave Output - Triangular
Amplitude(VP-P)
(V)
Time period
(ms)
Amplitude (VP-P)
(V)
Time period
(ms)
Input –sine wave Output - cosine
Amplitude(VP-P)
(V)
Time period
(ms)
Amplitude (VP-P)
(V)
Time period
(ms)
Differentiator
Input –square wave Output - Spikes
Amplitude (VP-P)
(V)
Time period
(ms)
Amplitude (VP-P)
(V)
Time period
(ms)
Input –sine wave Output - cosine
Amplitude (VP-P)
(V)
Time period
(ms)
Amplitude (VP-P)
(V)
Time period
(ms)
Precautions
Check the connections before giving the power supply.
Readings should be taken carefully.
Results
Inferences
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Questions
1. What are the problems of ideal differentiator?
2. What are the problems of ideal integrator?
3. What are the applications of differentiator and integrator?
4. What is the need for Rf in the circuit of integrator?
5. What is the effect of C1 on the output of a differentiator?
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4. Active Filter Applications – LPF, HPF (first order)
Aim: To design and obtain the frequency response of
i) First order Low Pass Filter (LPF)
ii) First order High Pass Filter (HPF)
Apparatus required
S.No Equipment/Component name Specifications/Value Quantity
1 IC 741 Refer page no. 2 1
2 Resistors
Variable Resistor
10k ohm
20kΩ pot
3
1
3 capacitors 0.01µf 1
4 Cathode Ray Oscilloscope (0 – 20MHz) 1
5 Regulated Power supply (0 – 30V),1A 1
6 Function Generator (1Hz – 1MHz) 1
Theory
LPF
A LPF allows frequencies from 0 to higher cut of frequency, fH. At fH the gain
is 3 db from maximum gain and after fH gain decreases at a constant rate with an
increase in frequency. The gain decreases 20dB each time the frequency is
increased by 10. Hence the rate at which the gain rolls off after fH is 20dB/decade or
6 dB/ octave, where octave signifies a two fold increase in frequency. The frequency
f=fH is called the cut off frequency because the gain of the filter at this frequency is
down by 3 dB from 0 Hz. Other equivalent terms for cut-off frequency are -3dB
frequency, break frequency, or corner frequency.
HPF
The frequency at which the magnitude of the gain is 0.707 times the maximum
value of gain is called low cut off frequency. Obviously, all frequencies higher than fL
are pass band frequencies with the highest frequency determined by the closed –
loop band width all of the op-amp. A HPF allows frequiences grater than lower cut of
frequency fL. At fL gain is 3 db down from maximum gain. The frequency f= fL is
called the lower cut off frequency.
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Circuit diagrams
Fig. 1: Low pass filter
Fig. 2: High pass filter
Design equations
• Chose a value of high cut off frequeinces fH =1/( 2πRC )
• Assume c <01 µF and calculate R using R= 1/(2πfHC) Ω
• Select value of R1 and RF depending on the desired pass band gain AF = 1+
(RF/R1)
First Order LPF: To design a Low Pass Filter for higher cut off frequency fH = 4 KHz
and pass band gain of 2
fH = 1/( 2πRC )
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Assuming C=0.01 µF, the value of R is found from
R= 1/(2πfHC) Ω =3.97KΩ
The pass band gain of LPF is given by AF = 1+ (RF/R1)= 2
Assuming R1=10 KΩ, the value of RF is found from
RF=( AF-1) R1=10KΩ
First Order HPF: To design a High Pass Filter for lower cut off frequency
fL = 4 KHz and pass band gain of 2
fL = 1/( 2πRC )
Assuming C=0.01 µF,the value of R is found from
R= 1/(2πfLC) Ω =3.97KΩ
The pass band gain of HPF is given by AF = 1+ (RF/R1)= 2
Assuming R1=10 KΩ, the value of RF is found from
RF=( AF-1) R1=10KΩ
Procedure
First Order LPF
1. Connections are made as per the circuit diagram shown in Fig.1.
2. Apply sinusoidal wave of constant amplitude as the input such that op-amp does
not go into saturation.
3. Vary the input frequency and note down the output amplitude at each step as
shown in Table (a).
4. Plot the frequency response as shown in Fig.3.
First Order HPF
1. Connections are made as per the circuit diagrams shown in Fig. 2.
1. Apply sinusoidal wave of constant amplitude as the input such that op-amp does
not go into saturation.
2. Vary the input frequency and note down the output amplitude at each step as
shown in Table (b).
4. Plot the frequency response as shown in Fig 4.
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Tabular Form Observations
Input voltage Vin = 0.5V
Table (a) First order LPF Table (b) First order HPF
Model graphs
Fig. 3: Frequency response of LPF Fig. 4:Frequency response of HPF
Frequency
(Hz)
O/P
Voltage(V)
Voltage
Gain
Vo/Vi
Gain
(dB)
Frequency
(Hz)
O/P
Voltage(V)
Voltage
Gain
Vo/Vi
Gain
(dB)
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Precautions
Check the connections before giving the power supply.
Readings should be taken carefully.
Results
Inferences
Questions
1. What is meant by frequency scaling?
2. How do you convert an original frequency (cut off) fH to a new cut off frequency
fH?
3. What is the effect of order of the filter on frequency response characteristics?
4. What modifications in circuit diagrams require to change the order of the filter?
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5. Active Filter Applications – BPF & Band Reject
(Wideband) and Notch Filters
Aim: To design and obtain the frequency response of
i) Wide Band pass filter
ii) Wide Band reject filter
iii) Notch filter
Apparatus required
Theory
Filter is a circuit that accepts certain band of frequencies and rejects other band of
frequencies
Band pass filter: A band pass filter has a pass band between two cutoff
frequencies fH and fL such that fH > fL. Any input frequency outside this pass band is
attenuated. There are two types of band-pass filters. Wide band pass and Narrow
band pass filters. We can define a filter as wide band pass if its quality factor Q <10.
If Q>10, then we call the filter a narrow band pass filter. A wide band pass filter can
be formed by simply cascading high-pass and low-pass filter the order of band pass
filter depends on the order of high pass and low pass filter.
S.No Equipment/Component name Specifications/Value Quantity
1 741 IC Refer page no 2 3
2 Resistors
Resistors
5.6kΩ
39kΩ
9
2
3 Resistors (20kΩ pot) 2
4 Capacitors
Capacitors
Capacitors
0.01µf
0.1µf
0.2µf
2
2 1
5 Regulated Power supply (0 – 30)V,1A 1
6 Function Generator (1Hz – 1MHZ) 1
7 Cathode Ray Oscilloscope (0 – 20MHz) 1
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Band Rejection Filter: The band-reject filter is also called a band-stop or
band-elimination filter. In this filter, frequencies are attenuated in the stop band while
they are passed outside this band. Band reject filters are classified as wide band-
reject narrow band-reject. Wide band-reject filter is formed using a low pass filter, a
high-pass filter and summing amplifier. To realize a band-reject response, the low
cut off frequency fL of high pass filter must be larger than high cut off frequency fH of
low pass filter. The pass band gain of both the high pass and low pass sections must
be equal.
Notch Filter or Narrow Band Reject Filter: The narrow band reject
filter, often called the notch fitter is commonly used for the rejection of a single
frequency. The most commonly used notch filter is the twin-T network .This is a
passive filter composed of two T-shaped networks. One T network is made up of two
resistors and a capacitor, while the other uses two capacitors and a resistor. The
passive twin-t network has a relatively low figure of merit can be increased
significantly by using active notch filter as shown in fig.3.The notch-out frequency is
the frequency at which maximum attenuation occurs and is given by
fN = 1/( 2πRC )
Circuit diagrams
Fig. 1: Wideband pass filter
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Fig. 2: Wideband reject filter
Fig. 3: Notch filter
Design
Band pass filter: To design a band pass filter having fH =400Hz and fL = 4KHz
and pass band gain of 2. As shown in Fig.1,the first section consisting of Op-
Amp,RF,R1,R and C is the high pass filter and second consisting of low pass filter.
The design of low pass and high pass filters.
Low Pass Filter Design
Assuming C’=0.01µf, the value of R’ is found from
R’ = 1/(2πfH C’) Ω =3.97KΩ
The pass band gain of LPF is given by ALPF = 1+ (R’ F / R’1) =2
Assuming R’1=5.6 KΩ, the value of R’F is found from R’F = ( AF-1) R’1=5.6KΩ
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High Pass Filter Design
Assuming C=0.01µf, the value of R is found from
R = 1/(2πfLC) Ω =39.7KΩ
The pass band gain of HPF is given by AHPF = 1+ (RF / R1 )=2
Assuming R1=5.6 KΩ, the value of RF is found from
RF = ( AF-1) R1=5.6KΩ
Band reject filter: To design a band reject filter with fH = 400Hz, fL = 4000Hz
and pass band gain of 2
Low Pass Filter Design
Assuming C’=0.01µf, the value of R’ is found from
R’ = 1/(2πfH C’) Ω =39KΩ
The pass band gain of LPF is given by ALPF = 1+ (R’ F / R’1 )=2
Assuming R’1=5.6 KΩ, the value of R’F is found from
R’F =( AF-1) R’1=5.6KΩ
High Pass Filter Design
Assuming C=0.01µf, the value of R is found from
R = 1/ (2πfLC) Ω =3.9KΩ
The pass band gain of HPF is given by AHPF = 1+ (RF / R1) =2
Assuming R1=5.6 KΩ, the value of RF is found from
RF = (AF-1) R1=5.6KΩ
Adder circuit design: Select all resistors equal value such that gain is unity.
Assume R2=R3=R4=5.6 KΩ
Notch Filter Design: fN = 400Hz
Assuming C=0.1µf,the value of R is found from
R = 1/ (2πfNC)=39 KΩ
Procedure
Wide Band Pass Filter
1. Connect the circuit as per the circuit diagram shown in Fig.1
2. Apply sinusoidal wave of 0.5V amplitude as input such that op-amp does not go
into saturation (depending on gain).
3. Vary the input frequency from 100 Hz to 100 KHz and note down the output
amplitude at each step as shown in Table (a).
4. Plot the frequency response as shown in Fig.4.
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Wide Band Reject Filter
1. Connect the circuit as per the circuit diagram shown in Fig.2
2. Apply sinusoidal wave of 0.5V amplitude as input such that opamp does not go
into saturation (depending on gain).
3. Vary the input frequency from 100 Hz to 100 KHz and note down the output
amplitude at each step as shown in Table( b).
4. Plot the frequency response as shown in Fig.5.
Notch Filter
1. Connect the circuit as per the circuit diagram shown in Fig 3
2. Apply sinusoidal wave of 2Vp-p amplitude as input such that opamp does not go
into saturation (depending on gain).
3. Vary the input frequency from 100 Hz to 4 KHz and note down the output
amplitude at each step as shown in Table( c).
4. Plot the frequency response as shown in Fig 6.
Observations
Input voltage (Vi) = 0.5V
Table(a) Band pass filter Table(b) Band Reject Filter
Frequency O/P
Voltage(V)
Gain
Vo/Vi
Gain in
dB
Frequency O/P
Voltage
Vo(V)
Gain
Vo/Vi
Gain in
dB
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Table(c) Notch filter
Input voltage=2Vp-p
Model graphs
Fig. 4 : Frequency response of Fig. 5 : Frequency response
wide band pass filter of wide band reject filter
Frequency O/P Voltage(V) Vo/Vi Gain in
dB
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Fig. 6: Frequency response of notch filter
Precautions
Check the connections before giving the power supply.
Readings should be taken carefully.
Results
Inferences
Questions
1. What is the relation between fC & fH, fL?
2. How do you increase the gain of the wideband pass filter?
3. What is the application of Notch filter?
4. What is the order of the filter (each type)?.What modifications you suggest for
the circuit diagram to increase the order of the filter?
5. What is the gain roll off outside the pass band?
6. What is the difference between active and passive filters?
7. What are the advantages of active filters over passive filters?
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6. IC 741 Oscillator Circuits
Phase Shift and Wien Bridge Oscillators
Aim: To design (i) phase shift and (ii) Wien Bridge oscillators for the given
frequency of oscillation and verify it practically.
Apparatus required
S.No Equipment/Component name Specifications/Value Quantity
1 IC 741 Refer page no. 2 1
2 Resistors
Variable Resistor
1.3 KΩ,3.18 KΩ
13KΩ, ,31.8 KΩ
500 KΩ pot
Each Three
Each one 1
3 Capacitors 0.1 µF
0.01 µF
3
2
4 Regulated Power supply (0 – 30V),1A 1
5 Cathode Ray Oscilloscope (0 -20MHz) 1
Theory
The function of an oscillator is to generate alternating current or voltage
waveforms.i,e. an oscillator circuits generates a repetitive wave form of fixed
amplitude and frequency without any external input signal. In oscillators positive
feedback is used. There are two conditions for oscillators
• magnitude of closed loop gain Aβ≥1
• Total phase shift of the loop gain Aβ=00 or 3600.
In the phase shift oscillator, out of 360o phase shift, 180o phase shift is
provided by the op-amp and another 180o is by 3 RC networks. In the Weinbridge
oscillator, the balancing condition of the bridge provides the total 360o phase shift.
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Circuit Diagrams
Fig. 1 : RC Phase shift oscillator
Fig. 2: Wien Bridge oscillator
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Design
1. Phase shift oscillator
To design a phase shift oscillator with fo =500 Hz
fo = 1/(2πRC 6 )
and gain= RF/R1= 29
Assuming C = 0.1 µF,the value of R is found from
R = 1/ (2π foC 6 ) = 1.3 KΩ
Take R1 = 10R =13 KΩ
RF = 29R1 (use 500K pot)
2. Wien Bridge Oscillator
To design a Wien bridge oscillator with fo =5 KHz
fo = 1/2πRC and RF = 2R1
Assuming C = 0.01 µF, the value of R is found from
R= 1/2πfc= 3.18 KΩ
Take R1 = 10 R=31.8 KΩ
RF = 2R1 (use 100K pot)
Procedures
1. Phase shift oscillator
1. Connect the circuit as per the circuit diagram shown in Fig.1
2. Observe the output waveform on the CRO.
3. Vary the potentiometer to get the undistorted waveform as shown Fig.a.
4. Measure the time period and amplitude of the output waveform.
5. Plot the waveforms on a graph sheet.
2. Wien Bridge Oscillator
1. Connect the circuit as per the circuit diagram shown in Fig.2
2. Observe the output waveform on the CRO.
3. Vary the potentiometer to get the undistorted waveform as shown in Fig.b
4. Measure the time period and amplitude of the output waveform.
5. Plot the waveforms on a graph sheet
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Waveforms
Fig.a: RC Phase Shift Oscillator Fig.b: Wien Bridge Oscillator
Tabular form and Observations
1. Phase shift oscillator
S.No Amplitude(VP-P) Time period
(ms)
Practical
frequency
(Hz)
Theoretical
frequency (Hz)
2. Wien Bridge Oscillator
S.No Amplitude(VP-P) Time period
(ms)
Practical
frequency
(Hz)
Theoretical frequency
(Hz)
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Precautions
Check the connections before giving the power supply.
Readings should be taken carefully.
Results
Inferences
[
Questions
1. What is an oscillator?
2. How do you change the frequency of oscillation in RC phase shift and Wien
bridge oscillators?
3. What are the applications of oscillators?
4. What is the advantage of using opamp in the oscillator circuit?
5. How do you achieve fine variations in fo ?
6. How do you achieve coarse variations in fo ?
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7. Function Generator using OPAMPs
Aim: To generate square wave and triangular wave forms by using OPAMPs.
Apparatus required
S.No Equipment/Component name Specifications/Value Quantity
1 741 IC Refer page no.2 2
2 Capacitors 0.01µf,0.001µf Each one
3 Resistors
Resistors
86kΩ ,68kΩ ,680kΩ
100kΩ
Each one
2
4 Regulated Power supply (0 – 30V),1A 1
5 Cathode Ray Oscilloscope (0 -20MHz) 1
Theory: Function generator generates waveforms such as sine, triangular, square
waves and so on of different frequencies and amplitudes. The circuit shown in Fig.1
is a simple circuit which generates square waves and triangular waves
simultaneously. Here the first section is a square wave generator and second
section is an integrator. When square wave is given as input to integrator it produces
triangular wave.
Circuit Diagram
Fig.1: Function generator
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Design
Square wave Generator
T= 2RfC ln (2R2 +R1/ R1)
Assume R1 = 1.16 R2
Then T= 2RfC
Assume C and find Rf
Assume R1 and find R2
Integrator
Take f= 1/(2π R3 Cf)
Assume Cf find R3
R4 =10 R3
Model Calculations
Square wave Generator
For T= 2 m sec
T = 2 Rf C
Assuming C= 0.01µf
Rf = 2.10-3/ 2.01.10-6
= 10 KΩ
Assuming R1 = 100 KΩ
R2 = 86 KΩ
Integrator
Assume Cf = 0.01µf
R3= 1/(2π f Cf) = 3.18KΩ take R3= 5KΩ
R4 = 50 KΩ
Procedure
1. Connect the circuit as per the circuit diagram shown above.
2. Obtain square wave at A and Triangular wave at Vo2 as shown in Fig.1.
3. Draw the output waveforms as shown in Fig.2(a) and (b).
Observations
Square Wave:
Vp-p = 26 V(p-p)
T = 1.8 msec
Triangular Wave:
Vp-p = 1.3 V
T= 1.8 msec
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Wave Forms
Fig. 2 (a): Output at ‘A’ Fig.2(b): Output at V02
Precautions
Check the connections before giving the power supply.
Readings should be taken carefully.
.
Results
Inferences
Questions
1. How do you change the frequency of square wave?
2. What are the applications of function generator?
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8. IC 555 Timer-Monostable Operation Circuit
Aim: To generate a pulse using Monostable Multivibrator by using IC555
Apparatus required
S.No Equipment/Component
name
Specifications/Value Quantity
1 555 IC Refer page no 6 1
2 Capacitors 0.1µf,0.01µf Each one
3 Resistor 10kΩ 1
4 Regulated Power supply (0 – 30V),1A 1
5 Function Generator (1HZ – 1MHz) 1
6 Cathode ray oscilloscope (0 – 20MHz) 1
Theory: A Monostable Multivibrator, often called a one-shot Multivibrator, is a
pulse-generating circuit in which the duration of the pulse is determined by the RC
network connected externally to the 555 timer. In a stable or stand by mode the
output of the circuit is approximately Zero or at logic-low level. When an external
trigger pulse is obtained, the output is forced to go high ( ≅ VCC). The time for which
the output remains high is determined by the external RC network connected to the
timer. At the end of the timing interval, the output automatically reverts back to its
logic-low stable state. The output stays low until the trigger pulse is again applied.
Then the cycle repeats. The Monostable circuit has only one stable state (output
low), hence the name monostable. Normally the output of the Monostable
Multivibrator is low.
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Circuit Diagram
Fig.1: Monostable Circuit using IC555
Design
Consider VCC = 5V, for given tp
Output pulse width tp = 1.1 RA C
Assume C in the order of microfarads & Find RA
Typical values
If C=0.1 µF, RA = 10k then tp = 1.1 mSec
Trigger Voltage must be greater than 1/3 Vcc let it be = 4 V
Procedure
1. Connect the circuit as shown in the circuit diagram.
2. Apply Negative triggering pulses at pin 2 of frequency 1 KHz.
3. Observe the output waveform and measure the pulse duration T high.
4. Compare it with given tp value.
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Waveforms
Fig. 2(a): Trigger signal (b) Output Voltage (c) Capacitor Voltage
Readings
Precautions
Check the connections before giving the power supply.
Readings should be taken carefully.
Results
Inferences
Trigger Output wave Capacitor output
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Questions
1. Is the triggering given is edge type or level type? If it is edge type, trailing or
raising edge?
2. What is the effect of amplitude and frequency of trigger on the output?
3. How to achieve variation of output pulse width over fine and course ranges?
4. What is the effect of Vcc on output?
5. What are the ideal charging and discharging time constants (in terms of R and C)
of capacitor voltage?
6. What is the other name of monostable Multivibrator? Why?
7. What are the applications of monostable Multivibrator?
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9. IC 555 Timer - Astable Operation Circuit
Aim: To generate pulse and square waveforms using IC555.
Apparatus required
S.No Equipment/Component
name
Specifications/Value Quantity
1 IC 555 Refer page no. 6 1
2 Resistors 3.6kΩ,7.2kΩ Each one
3 Capacitors 0.1µf,0.01µf Each one
4 Diode OA79 1
5 Regulated Power supply (0 – 30V),1A 1
6 Cathode Ray Oscilloscope (0 – 20MHz) 1
Theory
When the power supply VCC is connected, the external timing capacitor ‘C”
charges towards VCC with a time constant (RA+RB) C. During this time, pin 3 is high
(≈VCC) as Reset R=0, Set S=1 and this combination makes Q=0 which has
unclamped the timing capacitor ‘C’.
When the capacitor voltage equals 2/3 VCC, the upper comparator triggers the
control flip flop on that Q =1. It makes Q1 ON and capacitor ‘C’ starts discharging
towards ground through RB and transistor Q1 with a time constant RBC. Current also
flows into Q1 through RA. Resistors RA and RB must be large enough to limit this
current and prevent damage to the discharge transistor Q1. The minimum value of
RA is approximately equal to VCC/0.2 where 0.2A is the maximum current through the
ON transistor Q1.
During the discharge of the timing capacitor C, as it reaches VCC/3, the lower
comparator is triggered and at this stage S=1, R=0 which turns Q =0. Now Q =0
unclamps the external timing capacitor C. The capacitor C is thus periodically
charged and discharged between 2/3 VCC and 1/3 VCC respectively. The length of
time that the output remains HIGH is the time for the capacitor to charge from 1/3 VCC
to 2/3 VCC.
The capacitor voltage for a low pass RC circuit subjected to a step input of
VCC volts is given by VC = VCC [1- exp (-t/RC)]
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Circuit Diagram
Fig.1: 555 Astable Circuit
Design
Charging Time t c = 0.69 (RA + 2RB) C
Discharging Time t d = 0.69 (RB) C
Total time period T = 0.69 (RA + 2 RB) C
f= 1/T = 1.44/ (RA + 2RB) C
The maker of the 555 timer Signetics defined
Duty cycle (D) = td/T = RB/(RA+2RB)
For a given value of frequency assume C and Duty cycle then find RA, RB
Model calculations
Given f=1 KHz. Assuming c=0.1µF and D=0.25
∴1 KHz = 1.44/ (RA+2RB) x 0.1x10-6 and 0.25 =RB/ (RA+2RB)
Solving both the above equations, we obtain RA & RB as
RA = 7.2K Ω
RB = 3.6K Ω
Procedure
i) Pulse Generator
1. Connect the circuit as per the circuit diagram shown without connecting the
diode OA79.
2. Observe and note down the waveform at pin 6 and across timing capacitor.
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3. Measure the frequency of oscillations and duty cycle and then compare with
the theoretical values.
4. Sketch both the waveforms to the same time scale.
ii) Square wave generator
1. Connect the diode OA79 as shown in Figure to get D=0.5 or 50%.
2. Choose Ra=Rb = 10KΩ and C=0.1µF
3. Observe the output waveform, measure frequency of oscillations and the duty
cycle and then sketch the o/p waveform.
Waveforms
Fig. 2 (a) Pulse output (b) Capacitor voltage of Unsymmetrical square wave output
(c)Square wave output
Observations
Parameter Unsymmetrical Symmetrical
Voltage VPP
Time period T
Duty cycle
Precautions
Check the connections before giving the power supply.
Readings should be taken carefully.
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Results
Inferences
Questions
1. What is the effect of C on the output?
2. How do you vary the duty cycle?
3. What are the applications of 555 in astable mode?
4. What is the function of diode in the circuit?
5. On what parameters Tc and Td designed?
6. What are charging and discharging times
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10. Schmitt Trigger Circuits- using IC 741 & IC 555
Aim: To design the Schmitt trigger circuit using IC 741 and IC 555
Apparatus required
S.No Equipment/Component name Specifications/Value Quantity
1 IC 741 Refer page no. 2 1
2 555IC Refer page no 6 1
3 Cathode Ray Oscilloscope (0 – 20MHz) 1
4 Multimeter 1
5 Resistors 100 Ω
56 KΩ
2
1
6 Capacitors 0.1 µf, 0.01 µf Each one
7 Regulated power supply (0 -30V),1A 1
Theory
The circuit shows an inverting comparator with positive feed back. This circuit
converts orbitrary wave forms to a square wave or pulse. The circuit is known as the
Schmitt trigger (or) squaring circuit. The input voltage Vin changes the state of the
output Vo every time it exceeds certain voltage levels called the upper threshold
voltage Vut and lower threshold voltage Vlt.
When Vo= - Vsat, the voltage across R1 is referred to as lower threshold
voltage, Vlt. When Vo=+Vsat, the voltage across R1 is referred to as upper threshold
voltage Vut.
The comparator with positive feed back is said to exhibit hysterisis, a dead
band condition.
Hysteresis width VH = VUT-VLT
Circuit Diagrams
Fig. 1: Schmitt trigger circuit using IC 741
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Fig. 2: Schmitt trigger circuit using IC 555
Design
Vutp = [R1/(R1+R2 )](+Vsat)
Vltp = [R1/(R1+R2 )](-Vsat)
Vhy = Vutp – Vltp
=[R1/(R1+R2)] [+Vsat – (-Vsat)]
Procedure
1. Connect the circuit as shown in Fig.1 and Fig.2.
2. Apply an arbitrary waveform (sine/triangular) of peak voltage greater than UTP to
the input of a Schmitt trigger.
3. Observe the output at pin6 of the IC 741 and at pin3 of IC 555 Schmitt trigger
circuit by varying the input and note down the readings as shown in Table 1 and
Table 2
4. Find the upper and lower threshold voltages (Vutp, VLtp) from the output wave
form.
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Wave forms
Fig. 3(a) Schmitt trigger input wave form (b) Schmitt trigger output wave form
Observations
Table 1
Parameter Input Output
741 555 741 555
Voltage( Vp-p)
Time period(ms)
Table 2
Parameter 741 555
Vutp
Vltp
Precautions
Check the connections before giving the power supply.
Readings should be taken carefully.
Results
Inferences
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Questions
1. What is the other name for Schmitt trigger circuit?
2. In Schmitt trigger which type of feed back is used?
3. What is meant by hysteresis?
4. What are effects of input signal amplitude and frequency on output?
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11. IC 565- PLL Applications
Aim: To design a frequency multiplier using IC 565
Apparatus required
S.No Equipment/Component name Specifications/Value Quantity
1 IC 565 Refer page no. 8 1
2 IC 555 Refer page no. 6 1
3 Resistors 12KΩ,54.5 KΩ Each one
4 Capacitors
0.01µF
0.1 µF
10µF
2
1 1
5 Regulated power supply (0 -30V),1A 1
6 Cathode Ray Oscilloscope (0 – 20MHz) 1
Theory
The frequency divider is inserted between the VCO and the phase
comparator of PLL. Since the output of the divider is locked to the input frequency fIN,
the VCO is actually running at a multiple of the input frequency .The desired amount
of multiplication can be obtained by selecting a proper divide– by – N network ,where
N is an integer. To obtain the output frequency fOUT=2fIN, N = 2 is chosen. One must
determine the input frequency range and then adjust the free running frequency fOUT
of the VCO by means of R1 and C1 so that the output frequency of the divider is
midway within the predetermined input frequency range. The output of the VCO now
should be 2fIN . The output of the VCO should be adjusted by varying potentiometer
R1. A small capacitor is connected between pin7 and pin8 to eliminate possible
oscillations. Also, capacitor C2 should be large enough to stabilize the VCO
frequency.
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Circuit diagram
Fig.1: PLL as Frequency Multiplier
Design
If C= 0.01µF and the frequency of input trigger signal is 2KHz, output pulse
width of 555 in monostable mode is given by
1.1RAC = 1.2T =1.2/f
RA= 1.2/(1.1Cf)=54.5KΩ
fIN=fOUT/N
Under locked conditions,
fOUT = NfIN = 2fIN = 4KHz
Procedure
1. The circuit is connected as per the circuit diagram.
2. Apply a square wave input to the pin2 of the 565
3. Observe the output at pin4 of 565 under locked condition.
4. Give the output of 565 to the pin2 of 555 IC.
5. Observe the output of 555 at pin3.
6. Now give the output of 555 as feedback to the pin5 of the 565.
7. Observe the frequency of output signal fo at pin4 of 565 IC.
8. Draw the wave forms.
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Wave forms
Fig. 2(a): Input
(b): PLL output under locked conditions without 555
(c): Output at pin4 of 565 with 555 connected in the feedback
Observations
Parameter Input Output
Amplitude (Vp-p)
Frequency (KHz)
Precautions
Check the connections before giving the power supply.
Readings should be taken carefully.
Result
Inferences
DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING
IC APPLICATIONS LABORATORY
60
Questions
1. Out of capture and lock ranges, which is smaller?
2. What is the function of VCO in a PLL?
3. What does happen if frequency divider network -by- 4 is placed in the
feedback?
DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING
IC APPLICATIONS LABORATORY
61
12. IC 566 – VCO Applications
Aim: i) To observe the applications of VCO-IC 566
ii) To generate the frequency modulated wave by using IC 566
Apparatus required
S.No Equipment/Component Name Specifications/Value Quantity
1 IC 566 Refer page no.10 1
2 Resistors 10KΩ
1.5KΩ
2
1
3 Capacitors 0.1 µF
100 pF
1
1
4 Regulated power supply 0-30 V, 1 A 1
5 Cathode Ray Oscilloscope 0-20 MHz 1
6 Function Generator 0.1-1 MHz 1
Theory
The VCO is a free running Multivibrator and operates at a set frequency fo
called free running frequency. This frequency is determined by an external timing
capacitor and an external resistor. It can also be shifted to either side by applying a
d.c control voltage vc to an appropriate terminal of the IC. The frequency deviation is
directly proportional to the dc control voltage and hence it is called a “voltage
controlled oscillator” or, in short, VCO.
The output frequency of the VCO can be changed either by R1, C1 or the
voltage VC at the modulating input terminal (pin 5). The voltage VC can be varied by
connecting a R1R2 circuit. The components R1 and C1 are first selected so that VCO
output frequency lies in the centre of the operating frequency range. Now the
modulating input voltage is usually varied from 0.75 VCC which can produce a
frequency variation of about 10 to 1.
DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING