There are three types of RC oscillators, Wien Bridge, TwinT, and PhaseShift. The the simplest
oscillators is the Wien Bridge Oscillator. Fig 1 shows a typical Wien bridge oscillator. The circuit
relies on a series RC network and a parallel RC network causing a phase shift of 0 degrees at one
particular frequency at the non inverting input. Thus, taking the signal at the + input, through the
op
amp, through R and C and back to the + input causes a phase shift of 0 degrees at one particular
frequency.
Fig. 1
The feedback resistors Ra and Rb set the gain to maintain oscillation.
The Wien bridge oscillator can be understood most readily by first considering the transfer function
of the RC network that forms the feedback loop. Calculating V2/V1 we find
For wRC = 1 the signal at the input of the amplifier is exactly in phase with that at the output,
and if
the amplifier has a gain of at least 3 (to compensate for the factor 1/3 in V2/V1) the circuit will
oscillate with a frequency of
When the gain of the amplifier is slightly larger than 3, the output amplitude will grow until it
saturates the amplifier, when the gain is less than 3 it will decay until the oscillator stops.
An easy way of analysing this circuit is to consider the gain and phase shift caused by the Wien
bridge network (the series and parallel RC components) and ignore the other components in the
circuit, as shown in Fig 2. At a specific frequency, the phase shift caused by the series RC is offset
by an equal and opposite phase shift caused by the parallel RC, so the net phase shift is zero. When
this occurs, the circuit will oscillate.
Fig 2
The second common design is called a "TwinT" oscillator as it uses two "T" RC circuits
operated
in parallel. One circuit is an RCR "T" which acts as a lowpass filter. The second circuit
is a CRC "T" which operates as a highpass filter. Together, these circuits form a bridge
which is tuned at
the desired frequency of oscillation.
The signal in the CRC branch of TwinT filter is advanced, in the RCR  delayed, so they may
cancel one another for frequency of
if X = 2; if it is connected as a negative feedback to an amplifier, and X>2, the amplified becomes
an oscillator.
Fig 3
The TwinT is a bandstop RC circuit (or notch filter). It blocks all but the resonant frequency
in the negative feedback loop.
Oscillation cannot occur at frequencies above or below the resonant frequency.
TwinT Audio Oscillator
Fig 4
R1 = R2
R3 = 0.1 * R1
C2 = C3 = C
C1 = 2 * C
R4 = 3K3 (approx)
C4 = 50nF (approx)
Q1 = any NPN audio amplifier.
Vcc is not critical, 6 to 12Vshould work fine. Higher or lower voltages may also work.
Another common design is the Phaseshift oscillators. One of the simplest
implementations for this type of oscillator uses an operational amplifier
(opamp), three capacitors and four resistors, as shown in Fig 5.
Fig 5
The filter must be designed so that at frequencies above and below the oscillation frequency the
signal is shifted by either more or less than 180 degrees. This results in constructive superposition
for signals at the oscillation frequencies, and destructive superposition for all other frequencies.
The calculations are greatly simplified by setting all the resistors (except the negative feedback
resistor) and all the capacitors to the same values. In the diagram, if R1 = R2 = R3 = R, and C1 =
C2 = C3 = C, then:
Where:
f is the Output Frequency in Hertz
R is the Resistance in Ohms
C is the Capacitance in Farads
N is the number of RC stages and in our example N = 3
and the oscillation criterion is:
