DEPARTMENT OF ELECTRICAL ENGINEERING
ESE UNDERGRADUATE LABORATORY
ESE 205: Electrical Circuits and Systems I Laboratory
Lab: 4
Operational Amplifiers – Basic Characteristics and
Applications
Objective
The objective of this lab experiment is to learn how to use the operational amplifier (op-amp). In this experiment some of the basic characteristics of the op-amp would be examined and then some of its applications like the voltage follower and as a comparator will be experimented.
Pre-Lab Assignment
The Operational
Amplifier (Op Amp) is an extremely useful device, as we will see in this lab.
With the addition of a few external components, an extraordinary variety of
functions can be implemented.
The Op Amp is an active
element that needs to be supplied with power to operate. A common way to supply
this power is shown in Figure 1. Two power supply voltages are used, with equal
values denoted by Vcc and VDD (or ±VCC) (often in the
range of 5 V to 15 V). The common node between the supplies is the ground node.
The op amp’s output voltage is taken between the output terminal and the ground
node. The remaining two terminals are the input of the op amp.
An interesting property
of the op-amp is that the output voltage is only a function of the difference
of the two input terminals.

Figure 1: A common method of supplying power to op-amp

Figure 2: Top view of an op-amp DIP (dual in-line package) chip.
Figure 2 shows the top
view of widely used OpAmp type known as the 741. It comes in a package, with
metal pins that can be pushed into a breadboard such as the one you will be
using for this experiment. With the package viewed from above and positioned as
shown (note the dot on the left), the pin numbering is understood to be as
indicated. The pins that correspond to the input, output, and power supply
connections are shown. When the OpAmp is connected to other elements, extremely
small currents flow at its input terminals. For our purposes, these currents
can be assumed to be zero.
The most basic function of the op amp is the voltage amplification. However, the output voltage of a real op amp is limited to the range between certain limits that depend on the internal design of the op amp. As shown in Figure 3, when the output voltage tries to exceed these limits, clipping occurs.

Figure 3: For an op-amp, clipping occurs if the output voltage exceeds
certain limits
1. Inverting Amplifier:
Simulate the Inverting amplifier shown in Figure 4 in MultiSIM for Av =
-50.
-For opamp selection, use "Place Component" from menu and select LM741CH opamp
-

-Use following function generator settings
-
-When opening the scope window, notice how two channel displays have different color !. To enable different colrs, change the color of the wire connected to the channels of the scope.
Where for an Inverting amplifier,

Select the larger of the two resistors in the above gain equation to be
equal to 100 kΩ, and come up with a value for the other. Use a combination
of standard resistor values for the second resistor, such that your actual
value of Av is approximately within ±1% of the desired value.


Use the function generator to produce a sinusoid at the input of the
amplifier and use the two channels of the oscilloscope to view the input and
the output waveforms simultaneously. Set the amplitude of the function
generator to 200 mV and measure the output amplitude and the phase shift
between the input and output waveform at 10 Hz, 1 kHz, and 100 kHz.
Does the phase and/or amplitude of the amplifier output changes with
frequency?
What happens if you change the amplitude of the function generator to 1
V?
If you use either a 10 MΩ resistor or a 1 kΩ resistor for the
larger of the two resistors that determine Av, and adjust the other resistor so
that your actual Av is still within ±1% of the desired value of .50, will any of the
above results change?
2. Non-Inverting Amplifier:
Repeat 1 for the Non-Inverting amplifier configuration shown in Figure 5.
Take Av =50.
For an Non-Inverting amplifier,


In-lab Assignment
A. Equipment:
B. Procedure
Inverting
Amplifier:
Hook up the inverting amplifier of figure 6, with Rin = 10 k and Rf = 100 k. Using a 1 kHz sinusoidal input signal with an amplitude of approximately 1 V, look at the input and output.
Verify that the amplifier inverts. Measure the gain and compare with what you expect. Replace the 100 k feedback resistor with 10 k. What gain do you predict and observe now?

Figure 6: Inverting amplifier
Non –
Inverting Amplifier:
Set up the non-inverting amplifier circuit of figure 7 with R1 = 10 k. With a 1 kHz sinusoidal input, measure the gain with R2 = 100k and with R2 = 10k. Compare with what you expect. Verify that the amplifier is non-inverting.

Figure 7: Non – inverting amplifier
Voltage
Follower:
As shown in figure 8, connect the output of the op-amp directly to the ‘-‘input and connect the output of the function generator to the ‘+’ input of the op-amp.
After turning on the power, confirm that the input and output signals are identical and that the voltage follower is non-inverting. Record the input and output amplitudes.

Figure 8: 741 as a voltage follower
Comparator:
With no negative feedback, the saturated output that results allows the op-amp to be used as a voltage comparator – a circuit that tells you whether an input voltage is higher or lower than a ‘threshold’ voltage. Since op-amps are not specifically engineered for open loop operation, it is not a very good voltage comparator, but in some situations an open loop 741 comparator is perfectly adequate.
Start by applying a 1 kHz sine wave to the input (pin 2) and ground pin 3. Observe what the circuit is doing.
Now raise the input frequency to 100 kHz. Notice that the output ‘square wave’ is not very square.
For each case studied, sketch the output waveform and measure the output amplitude and DC offset. Explain your measurements.

Figure 9: 741 as a comparator
Capture the output waveforms wherever necessary to be pasted in your lab notebook as well as your report.
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Created by Jan Van der Spiegel:
Updated by Jorge Juan Santiago