Wien’s Bridge Audio Frequency Oscillator
Points : wien’s bridge audio frequency oscillator
It is one of the most popular type of oscillators used in audio and sub-audio frequency ranges (20HZ -
20 KH). This type of oscillator is simple in design, compact in size, and remarkable stable in its frequency
output. Furthermore, its output is relatively free from distortion and its frequency can he varied easily.
However, the maximum frequency output of a typical wien bridge oscillator is only about 1 MHz.
The circuit arrangement of a wien bridge oscillator is shown in fig. It is essentially a two — stage amplifier
with R.C bridge circuit. R.C bridge circuit (Wien bridge) works as the feedback network between the input and
output.
In the bridge circuit R1, c1, R3, R4 and R2 are in parallel
with C2 form the four arms. From the analysis of the bridge circuit it is obvious that the bridge will
be balanced only when:
Thus we see that in a bridge circuit the output will be in phase with the input only when the bridge is balanced
i.e, at resonant frequency given by expression (iii).
So this bridge circuit can be used as feedback for an oscillator, provided
that the phase shift through the amplifier is zero. This requisite condition is
achieved by using a two stage amplifier, as illustrated in the fig. In this
arrangement the output of the second stage is supplied back to the feedback
network and the voltage across the parallel combination C2 R2 is fed to the input of the
first stage. Transistor T1, serves as an oscillator and amplifier whereas the transistor T2
as an inverter to cause a phase shift of 1800 degree. The circuit use positive and negative feedbacks. The
positive feedback is through the voltage divider to R1, C1, R2, C2 to
transistor T, and negative feedback is through the
voltage divider to the input of transistor T2. Resistors R3 and R4 are used to
stabilize the amplitude of the output.
The two transistors T1, & T2 thus cause a total phase shift of 360° degree and ensure proper
positive feedback. The negative feedback is provided in the circuit to ensure constant output over a range of
frequencies. This is achieved by taking resistor R4 in the form of a temperature sensitive lamp, whose resistance
increases with the increase in current. In the amplitude of the output tends to increase, more current would
provide more negative feedback. Thus the output would regain its original value.) A reverse action would take
place in case the output tends to fall.
The continuous frequency variation in this oscillator can be had by varying the two capacitors C1 and
C2 simultaneously. These capacitors are variable air-gang capacitors. We can change the frequency range
of the oscillator by switching into the circuit different values of resistors R1 & R2.
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