Author Name: Vasilis Leandrou
OBJECTIVES
This report aims to:
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To explain an inverting operational amplifier circuit.
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To explain a non-inverting operational amplifier circuit.
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To find out the operational amplifier voltage follower.
BACKGROUND THEORY
In this experiment will be used the 741 operational amplifier, 3DC power supplies, an analog signal generator, a dual-trace oscilloscope and resistors (1ΜΩ, 100ΚΩ, 10ΚΩ, 4.7ΚΩ, 2.2ΚΩ, 1ΚΩ, 470Ω)
· The operation amplifier is an electronic circuit, increasingly important. It can be used as a circuit building block by focusing on its terminal behavior.
· Power supplies gives a source of power, rated as maximum voltage and current output
· The oscilloscope is an instrument that will display the variation of a voltage with time on a flat screen monitor.
EQUIPMENT and COMPONENTS USED
· Dual Trace Oscilloscope (Brand: HAMEG, Model: HM 203-6, Serial Number: 46/87 Z33418)
· Function generator (Model: TG 550)
· Power supply (GW GPS-3030PP, Serial Number: EG820606)
· 741 operational amplifier
· Resistors (1ΜΩ, 100ΚΩ, 10ΚΩ, 4.7ΚΩ, 2.2ΚΩ, 1ΚΩ, 470Ω)
EXPERIMENTAL METHOD
Part 1
An inverting amplifier circuit. The dual-trace oscilloscope was connected onto an operational amplifier and the signal generator was replaced with a dc power supply witch is verified that the inverting amplifier is a dc amplifier. The resistance of Rf was changed and the output voltage and the gain was measured (table 1).
The inverting amplifier voltage gain Av is equal with the feedback resistor divisible with the input resistor.
Av = -Rf / Rs
Part 2
A non inverting amplifier. The dual-trace oscilloscope was connected onto an operation amplifier and the signal generator was replaced with a dc power supply which is verified that is used as a non-inverting amplifier. The resistance of Rf was changed and the output voltage and the gain was measured (table 2).
The non-inverting amplifier voltage gain is determined by the equation:
Av= 1+ (Rf / Rs)
Part 3
Operational amplifier voltage follower. To find out the operational amplifier voltage follower, a circuit was connected with Vs = 5Vpk at 1 KHz. The output voltage V0 is measured. The procedure was repeated with Vs = 10Vdc and Vs = 2Vpk square wave.
OBSERVATIONS
Table 1 inverting amplifier
Rf(ohms) |
V0(volts) |
Av=V0/Vs |
Av=Rf/Rs |
different% |
471Ω |
50mV |
0.5 |
0.48 |
4% |
1ΚΩ |
100mV |
1 |
1.02 |
2% |
2.2ΚΩ |
225mV |
2.25 |
2.24 |
0.45% |
4.69ΚΩ |
480mV |
4.8 |
4.74 |
1.25% |
10.1ΚΩ |
1000mV |
10 |
10.32 |
3.2% |
94.5ΚΩ |
10.000mV |
100 |
101.7 |
1.7% |
Table 2 non-inverting amplifier
Rf(ohms) |
V0(volts) |
AV=V0/Vs |
Av=1+Rf/Rs |
different% |
471Ω |
150mV |
1.5 |
1.48 |
1.3% |
1ΚΩ |
200mV |
2 |
2.02 |
1% |
2.2ΚΩ |
340mV |
3.4 |
3.24 |
4.5% |
4.69ΚΩ |
600mV |
6 |
5.74 |
4.3% |
10.1ΚΩ |
1150mV |
11.5 |
11.32 |
1.56% |
94.5ΚΩ |
10000mV |
100 |
102.7 |
2.7% |