After all the epic discussions-:) about the Wien bridge oscillator...

https://www.researchgate.net/post/What_is_the_basic_idea_of_Wien_bridge_oscillator_How_does_it_operate

...I have finally arrived at the conclusion that we have to consider the bare Wien network as a key point of understanding the Wien oscillator. For this purpose, we have to reveal the role of each element constituting the whole network. Here are my speculations.

The Wien network consists of four elements - C1, R1, C2 and R2, but they can be grouped into two parts (impedance elements) - the lower part consists of the two connected in parallel C1 and R1; the upper part consists of the two connected in series C2 and R2. Thus, the Wien network can be thought as of a frequency- or time-dependent voltage divider. Let's think freely over and even dream about this ubiquitous arrangement to stir our imagination...

The voltage divider configuration consists of two impedances connected in series. The input voltage is applied across the whole network. The output voltage is taken between the common point and some reference point: the ground, the voltage supply rail or a middle point (virtual ground). In the last case, we obtain a bridge configuration (the Wien bridge in our case).

FREQUENCY DOMAIN. The two elements (resistive, nonlinear, reactive, etc.) of the voltage divider configuration have an opposite influence over the transfer ratio and the output voltage. If only one of them is frequently dependent (a capacitor), it will act as "loosing" or "pulling" element when the frequency increases from zero up to infinity. Thus we obtain the classic integrating (low-pass) and differentiating (high-pass) circuits.

Now assume both the elements are frequency-dependent and we have taken the voltage drop across the lower element as an output (the case of the Wien bridge oscillator). When the frequency increases, the impedance of the lower element decreases up to zero and the ratio (the output voltage) decreases up to zero as well. Contrary, if the frequency decreases, the impedance of the upper element increases up to infinity and the ratio (the output voltage) decreases up to zero again. Only at some ("resonant") frequency the ratio of this frequency-dependent voltage divider reaches its maximum of 1/3 and the circuit behaves as some "mixture" of integrating and differentiating circuits (band-pass). It is interesting to see how such a behavior is achieved... to imagine how Wien was thinking when inventing this clever passive circuits... to put ourselves in his place...

If the two elements had opposite frequency-dependent behavior (a capacitor and an inductor), there was no a problem to create a band-pass voltage divider. The problem here is that we have only one kind of a frequency-dependent element - a capacitor, having a different behavior at different frequencies: it has a low impedance at high frequency and high impedance at low frequency. Then, how do we make it to have the same behavior (not to pass the signal) at both the frequencies - high and low?

If we look closely at the Wien network, we can discern an integrating (low-pass) circuit or a differentiating (high-pass) circuit or both the elementary circuits inside it. First, we can think of it as of an integrating circuit R2-C1 that is "neutralized" at extremely low frequencies by connecting the capacitor C2 in series with the resistor R2 and the resistor R1 in parallel to the capacitor C1. Then, with the same success, we can think of it as of a differentiating circuit C2-R1 that is "neutralized" at extremely high frequencies by connecting the resistor R2 in series with the capacitor C2 and the capacitor C1 in parallel to the resistor R1.

Thus, at the very high frequencies, the behavior of the upper capacitor C2 is reversed and made similar to the behavior of an inductor by connecting in series the resistor R2 (the capacitive reactance has gradually disapeared with the frequency increase and the resistance R2 has gradually dominated). At the very low frequencies, the behavior of the lower capacitor C1 is reversed and made similar to the behavior of an inductor by connecting in parallel the resistor R1 (the capacitive reactance has gradually increased up to infinity with the frequency decrease and the resistance R1 has gradually dominated).

So, this was the great Wien's idea - to transmute a capacitor into an "inductor": at the very high frequencies - by connecting in series a resistor; at the very low frequencies - by connecting in parallel a resistor. Am I right?

TIME DOMAIN. It is even more interesting to investigate the Wien network operation through the time. I would even build a "real-time simulation" arrangement to visualize the operation extremely slowly, in a human friendly manner, like this one:

http://en.wikibooks.org/wiki/Circuit_Idea/Walking_along_the_Resistive_Film#How_to_visualize_the_voltage_diagram_on_the_screen

For this purpose, use high resistances (e.g., 100 kom) and large capacitances (e.g., 100 μF) to obtain an extremely low "resonant" frequency (about 0.01 Hz). Then, drive the network with a varying sine wave voltage source with an extremely low frequency (it is interesting to vary the voltage manually trying to keep a sine wave). Next, connect three Microlab analog inputs (ADCs): the first - to the input voltage; the second - to the voltage of the common point between the upper elements R2 and C2; the third - to the common point between the two network parts (the common point of R1, C1 and R2). Finally, write a program that continuously measures the voltages and draws voltage bars over the respective elements representing the voltages across them like this diagram (in addition, it draws current loops):

http://commons.wikimedia.org/wiki/File:Chung_3_1000.jpg

My next explanations are closely related to the Lutz's considerations about the network operation, e.g. this one: "...However, always: V(P)

More Cyril Mechkov's questions See All
Similar questions and discussions