Introduction
In many
electronic circuits, the signals (voltage
differences) that are generated and manipulated are very small. Therefore, amplification is often
essential. When playing a CD, for
instance, the signals generated in the CD player are quite small and will not
adequately drive a speaker system. The
signals from the CD player are therefore passed into the stereo amplifier
(which often comes as a tuner/amplifier combination in modern home stereo
systems). The heart of the stereo
amplifier is the operational amplifier, or op-amp, which takes low level
voltage signals as inputs and produces large output voltages that vary linearly
with the input voltage.
Operational Amplifiers
The op-amp is a
simple example of an integrated circuit.
The common 411 op-amp used in this laboratory contains 24 transistors on
a single silicon chip. Many integrated
circuits are much larger: a computer's
microprocessor can contain several million separate elements. Each transistor is a three terminal
semiconductor device that controls a large current with a small one. If you later study electronics, you will
learn about transistors. In this course,
we will omit that stage and show how the functioning of op-amp circuits can be
understood without knowing anything about the individual transistors of which
op-amps are composed. You need only
understand a few basic principles (explained below) and Kirchoff's circuit
laws. Our reason for doing this lab is
to show you how practical problems can be solved using electronic devices. These days, most scientists solve practical
instrumentation problems using op-amps and other integrated circuits rather
than discrete components.
An
op-amp has three main terminals. The
circuit symbol for an op-amp is shown in figure 1. The V- input is called the
inverting input, the V+ input is called the non-inverting input, and
Vout is the output voltage.
All voltages are measured relative to the ground line of the power supply
for the op-amp. All op-amps need a power
supply in order to provide the amplification, since without a voltage higher
than the input voltages it would be impossible to produce amplification. Generally the power supply is provided by
connections at +15 V and -15 V to the op-amp.
(Note that by convention, these power supply connections are not shown
on the circuit symbol for the op-amp.
However, you must always connect them up in the lab.) The supply voltages determine the maximum
output voltage range of the op-amp, and if Vout reaches one of the
supply voltages the op-amp is said to be in "saturation". This situation is to be avoided since if the
op-amp is in saturation, its output cannot be varying linearly with the inputs.
Figure 1: Op-amp inputs and output
The op-amp will
amplify both AC and DC signals, although there is a high frequency f3dB
(analogous to the f3dB or “cutoff frequency of a low-pass filter)
determined by the type of op-amp; frequencies beyond this value will be
amplified less and less as the frequency increases. We describe the signal
amplifying properties of the op-amp by giving its gain, and the ratio between the output signal and the input
signal. In the so-called "open
loop" configuration shown in figure 1, the output voltage is given by
where the open loop voltage gain A0 characterizes
the op-amp. Note that the voltage
difference between the inputs is
amplified and not the voltage between an input and ground. If you add 5 volts to both inputs, this does
not affect the output at all! Equation 1
makes it clear why V-
is called the "inverting" input; it contributes negatively to the
output signal.
The input
impedance of an op-amp is typically 106 W although it can be as high as 1012 W in some models. The output impedance is usually very
small. The gain A0 is
extraordinarily high, typically 106 at low frequencies, so that an op-amp hooked
up solely with two inputs and its supplies would almost certainly be in saturation
(a voltage difference of only 15 microvolts between the inputs would be
sufficient to cause saturation). By
using "feedback" (see below), this high gain can be controlled and
made useful.
Feedback
Because the
op-amp has such a huge open loop gain A0, it is always used with a feedback network that controls the
inputs by returning some voltage from the output to the input. This reduces the effective gain, but it also
causes the amplification to be nearly independent of frequency up to much higher
frequencies than the open loop f3dB mentioned above.
The term
feedback refers to configurations in which a fraction of the output voltage is
returned (it is "fed back") to one of the inputs (see figure 2). Thus, the output Vout depends upon
itself, as well as the input to the circuit, Vin. (If you find this idea confusing, you are not
alone. The US Patent Office refused to
grant its inventor a patent for this extremely important engineering concept
because it didn't believe his idea would work!)
Feedback can be positive (returned to the non-inverting input) or
negative (returned to the inverting input), but negative feedback is used
primarily in analog circuits because it yields stable, controllable outputs,
and we will concentrate on it. For positive
feedback, an increasing output Vout
Negative feedback--stable Positive
feedback--unstable
Figure 2: Feedback
drives the inputs even further positive, resulting in a
still more positive Vout. (A similar
argument can be made that once Vout swings negative, it will result
in a large negative swing.) As a result,
the device will always be in saturation.
While this can be useful for some purposes (e.g. for making oscillators and in digital circuits), we shall
concentrate on "negative feedback" here. To make the idea more comprehensible, we will
first consider some non-electronic examples of feedback.
EXAMPLES OF FEEDBACK
Steam
engines were equipped with devices called governors to make sure their pressure
did not exceed a safe level. The
governor consisted of a valve connected to an array of spinning weights. The valve opened wider as the weights spun
more quickly. Steam from a vent
controlled by the valve made the weights spin around: if the pressure rose, the weights would spin
more quickly. In turn, the weights would
open the valve more, thereby lowering the pressure. This represents a case of negative feedback
because the output (the pressure in the steam engine) was made to decrease automatically
if it became larger than the desired value.
The
concept of feedback has extremely wide applications to other fields of study,
including mathematical biology and economics.
For example, predator-prey relationships rely upon several feedback
loops that determine the stable size of populations. If the number of predators (the system's
output) increases, then the number of prey animals (the input) will
decrease. The negative feedback in this
system occurs because an increase in the output (predator population) results
in a decrease in the input (prey population).
There will in general be an equilibrium ratio of populations as a result
of the stabilizing influence of the negative feedback, with, of course, many
other factors entering in to establish their exact sizes.
In
another example, computerized trading of stocks on the stock market represents
a prime example of the pernicious effects of positive feedback. Extremely large investors, such as pension
funds, can buy and sell stocks using computer programs set to make trading
decisions based on the behavior of a market index, such as the Dow Jones
Industrial Average. These trading
decisions are the system's inputs. When
the stock market index (the system's output) begins to drop, these programs are
designed to quickly sell off stocks in order to minimize investors'
losses. However, a large investor can
further depress the stock market index by selling off its stocks (i.e. the system has positive
feedback). This system can lead to wild
oscillations, or even a crash, should many large investors use such programs
during a period of sharply falling prices.
The Securities and Exchange Commission decided to regulate computerized
trading after this practice was implicated in the major crash of 1987.
Golden Rules
One can show
mathematically that the results of feedback in op-amps circuits are summarized
by two "golden rules", which we will take as our starting points for
figuring out how op-amp circuits will function:
1)
The output of the op-amp attempts to do whatever
is necessary to make the voltage
difference between the inputs almost equal to zero. (That's the function of high gain of the
amplifier and the negative feedback; if the output voltage rises too much, it
drives the input voltage difference down.)
The voltage difference between the inputs is so close to zero that we
can assume that it really is zero in analyzing circuits. It turns out that if A=106, then the
error in this assumption is only about one part in a million.
2)
The inputs draw almost no current, because the
input impedance of the transistors attached to the inputs are very high.
Figure 3: Inverting amplifier circuit (the triangle at
the bottom denotes power supply ground).
Using the
golden rules, the negative feedback "inverting amplifier" circuit
shown in figure 3 can be analyzed. From
golden rule number 1, the voltage at the inverting input must be at ground
because V+ is at ground.
(The inverting input isn't actually connected
to ground, rather the internal circuitry of the op-amp labors to keep it very
near ground. We call such a voltage a virtual ground.) From golden rule number 2, all of the
current through R1 must flow through RF, because no
current flows into the op-amp inputs.
We arbitrarily take the direction of the conventional (positive) current
to be to the right. Then applying Kirchoff's laws gives
This means that you can choose the gain by selecting the
values of the resistors! Also, the gain
is not dependent on the details of the particular op-amp (e.g. the exact value
of the open loop gain A0), but rests only on the open loop
gain being large, and on the values of the resistors. (The largeness of A0 is the
underlying justification for Golden Rule 1.)
Since the output is negative for positive inputs, the amplifier called
an inverting amplifier.
Experimental Procedure
Experiment 1: Op-amp
in an open loop configuration
You will be
using the LF411 op-amp in today's lab.
(The F refers to the original manufacturer, Fairchild, and the other
numbers specify one of many different integrated circuits made by this
company.) It comes as a eight-legged
DIP ("dual in-line package") IC (integrated circuit) shown in figure
4. The LF 411 has been inserted into
your breadboard for you.
Figure 4: Connections for the LF 411 op-amp (top view)
The
"offset null" connections will not
be used here; their purpose is to allow the user to make small adjustments if
desired so that the output is precisely zero when the input voltage difference
is precisely zero.
Figure 5: Open loop circuit (the triangle at the bottom
is power supply ground).
1)
Assemble the circuit shown in figure 5. Here a voltage divider is used to provide the
op-amp with an input voltage (relative to power supply ground) varying from
+15V to -15V, with a potentiometer controlling the exact value.
2)
Use a DMM to adjust your input voltage until it
is very close to zero. Notice that the
output voltage is far from zero because of the very high open loop gain of the
op-amp. Try adjusting the input and sketch
the output voltage as a function of the input voltage. Explain briefly why your graph looks the
way it does.
Experiment 2: Inverting Amplifier with negative feedback
Figure 3
(presented earlier) employs negative feedback (from Vout to V-)
to give a stable gain that is controlled by the ratio of two resistors. In this portion of the lab you will construct
an op-amp circuit with negative feedback.
1)
Set up the circuit shown in figure 3 using a 411
op-amp. Remember to connect the +/-15V
DC supply, and also the ground (common) from the DC supply! Use your function generator's sine wave
setting and the LO output set to a very low voltage to supply Vin. The feedback is set up by connecting pin 6 to
pin 2 with RF. Choose RF=100
KW, and use a resistor for R1
that gives a closed-loop gain of 100.
2)
Plot both the input and output voltages as a
function of time on your oscilloscope, using a roughly 1 kHz signal. You should start with an extremely low
amplitude input signal to see a clear sine wave output. Sketch this display, carefully noting the
amplitudes and phase relationships of the two signals. Determine the gain of your circuit from this
data.
3)
Now, try increasing the amplitude of your input
signal until you start to see saturation (i.e. flattening as the output reaches
a maximum positive or negative value) at
some times. How large an input is
required to do this? What determines
whether the output is saturated?
Experiment 3: Weighted summing circuit
Op-amps can be
used to do mathematical computations.
For example, they can be used to compute the sum of many inputs, with
each one multiplied by a selectable gain.
For example, the output of the circuit shown in figure 6 is given by the
following expression:
.
This can easily be generalized to an arbitrary number of
inputs by adding terms to the equation.
Figure 6: Weighted summing circuit.
Another useful
function of an op-amp is to compute the integral or derivative of an input
signal. It may be surprising to realize
that all the integrals we compute mathematically can be calculated
electronically by the simple op-amp circuit shown above. Figure 7 shows an op-amp circuit for which
the negative feedback is now through an RC circuit rather than just a resistor. From the golden rules, the current flowing through
R and C must be equal just as for the resistors in figure 3 above. (Note that RS carries
insignificant current because you will choose it to be very large (>>10´)
compared to R. It is there to discharge
the capacitor for very long times when the input voltage is turned off, or if
the function-generator has a DC offset.
Otherwise, charge will build up gradually and saturate the op-amp.) So
Therefore, the output voltage at a given time is the
integral of the input voltage from some initial time (when the feedback was
connected) to the present time (t).
However, in
this case, a small deviation from ideal behavior in the op-amp can cause
problems. As you will have noted
earlier, there can be a small offset voltage between the inputs of an op-amp
even when the output is zero. In an
amplifier circuit (e.g. experiment
2), this can often be ignored. In an
integrator, however, it is a real problem, because the small constant offset
voltage will be integrated to produce a gradually growing output that
eventually dominates over the desired integration of the real input signal. This
linearly increasing spurious output is manifested by a gradual accumulation of
charge on the capacitor. The function of
RS is to allow this charge to leak off slowly. This prevents the "drift", but it
also means that the circuit will not act as an integrator for signals whose
frequencies are too low (smaller than 1/RSC).
A differentiator can be constructed by small modifications of this
circuit, but we shall not do so here.
1)
Assemble the circuit shown in figure 7 and test
its performance at a frequency w that
is large compared to 1/RSC by using an input signal from the LO
output of your function generator. Try
1/RsC 100 s-1
with C = 0.1 µF, and adjust the frequency so that the output signal has a
convenient amplitude. To get a
substantial gain you will need w
<< 1/RC. (Apply Eq. 6 to a
sinusoidal input signal.) Compare the
amplitudes of the input and output against the theoretical prediction.
2)
Use a variety of input signals from your
function generator, starting with a square wave. Be sure to try out sine waves and triangle
waves too. Sketch sample input and
output signals in your brief report.
Explain your results qualitatively.
3)
Also check one case (say, the square wave) as a
function of frequency. Find out what
happens if the frequency is made either too high or too low.
In this
experiment you have explored only a few of the hundreds of useful tasks that op-amps can perform. Other circuits that can be easily built with
op-amps include current-to-voltage converters; oscillators of various kinds;
precision current sources; precision AC-to-DC converters; filters of various
kinds; timers; log generators (output is the log of the input); precision power
supplies. Most of these circuits are far
superior to circuits that can be constructed from individual semiconductor
devices. The fundamental reason is the
high gain and high input impedance of the op-amp.
A stereo amplifier is an operational amplifier, this information was unknown to me. You have shared valuable information about the operational amplifier, but because of the background color, some figures are unable to understand clearly. Hope you will change it soon. By the way, Here you use LF411 Op-Amp IC and recently I read an article that was on 741 operational amplifiers both are similar.
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