EE 212L: Wien Bridge and Phase Shift Oscillators
Background: The importance of oscillators in electronics is
illustrated in this excerpt from The Art of Electronics by
Horowitz and Hill:
Within nearly every electronic instrument it is essential
to have an oscillator or waveform generator of some sort. Apart from
the obvious cases of signal generators, function generators, and pulse
generators themselves, a source of regular oscillations is necessary
in any cyclical measuring instrument, in any instrument that initiates
measurements or processes, and in any instrument whose function
involves periodic states or periodic waveforms. For example,
oscillators or waveform generators are used in digital multimeters,
oscilloscopes, radiofrequency receivers, computers, every computer
peripheral (tape, disc, printer, alphanumeric terminal), nearly every
digital instrument (counters, timers, calculators, and anything with a
"multiplexed display"), and a host of other devices too numerous to
mention. A device without an oscillator either doesn't do anything or
expects to be driven by something else (which probably contains an
oscillator). It is not an exaggeration to say that an oscillator of
some sort is as essential an ingredient in electronics as a regulated
supply of dc power.
Wien bridge and phase shift oscillators are good ways to produce
low-distortion sinusoidal signals at low to moderate
frequencies. These oscillators are circuits in which the output is
equal to the input at a given frequency. For such a circuit, when the
output is connected back to the input, a self-sustaining oscillation
takes place at the given frequency.
Pre-lab:
- Find the transfer function
Vout(jω)/Vin(jω) for the
circuit shown in Figure 1 of the lab (where complex frequency
variable s = jω can be substituted for ease of
analysis.) Calculate values for R and C such that the phase shift
between the output and input is zero for an input frequency of
10kHz. What is the amplitude ratio (gain) of the output to the
input at this frequency.
- The RC network in figure 3 of the lab can produce a phase shift
of 180° at a desired frequency. Calculate this frequency for
the network values given. (Recall a 180° phase shift
corresponds to the transfer function
Vout(jω)/Vin(jω) being a
real negative number.) What is the gain of the circuit?
Laboratory Procedure:
- Build the following circuit using the component values
determined in the prelab. With a sinusoidal input, observe the
phase shift between input and output. Find the frequency at which
the phase shift is zero and compare to the design frequency of
10kHz. Determine the ratio of the output to the input amplitude
and compare to the value calculated in the prelab.
- Connect the above circuit to a non-inverting amplifier based
upon a 355/356 op-amp. This is depicted in figure 2 where its
noted that the amplifier symbol (triangle) represents the
non-inverting amplifier circuit. Adjust the gain of the amplifier
and the frequency of the function generator until the amplitude
and the phase of the output equal those of the input. (Include a
precision (multi-turn) pot in the amplifier circuit to make the
gain adjustable.)
- When the output is the same as the input, disconnect the signal
generator and connect the output of the circuit to the input. With
a little adjustment of the gain, the circuit should oscillate,
producing a nice sine wave. Measure the frequency, and compare to
the design frequency and the frequency measured in Part 1.
- The RC network in Figure 3 can produce a phase shift of 180° at
a desired frequency. In the prelab, you calculated
this frequency for the component values given. Build the
circuit. With a sinusoidal input, adjust the frequency of
the function generator until the phase shift is 180°. Compare the
frequency that yields 180° of phase to the frequency computed in
the prelab. What is the gain of the circuit? How does this compare
to your prelab
result?
- To make an oscillator, we need 0° or 360° of phase shift.
Supply the extra phase shift with an inverting op-amp
amplifier. The op-amp circuit can also supply the gain needed to
make the input and output equal. Design and build the amplifier
with adjustable gain. (The final 1 kΩ should become the input
resistor, as it effectively goes to ground in both cases - compare
Figure 3 and Figure 4.) Adjust the gain and frequency until
vout = vin.
- Complete the oscillator by again connecting the input to the
output. Adjust the gain for an undistorted sine wave. Measure the
frequency. How does this compare to the design frequency?
@copy; Copyright 2003 New Mexico Institute of Mining and Technology
Revised MAR2015