Oscillator problem, explanation needed

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Discussion Overview

The discussion revolves around the Colpitts oscillator circuit, focusing on its simulation, component values, and the conditions necessary for oscillation. Participants seek clarification on various aspects of the circuit, including component roles, resonant frequency, and measurement techniques.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions whether the circuit is complete and expresses uncertainty about the role of certain components, particularly capacitors and resistors.
  • Another participant clarifies that R3, R4, and R5 are resistors, not capacitors, and suggests grounding the circuit for proper operation.
  • A participant mentions achieving oscillation in their simulation but seeks guidance on confirming the oscillation frequency.
  • There is a discussion about the Q factor and its dependence on various resistances, with one participant noting that the resistance in the Q factor formula may include the coil wire resistance and other parallel resistances.
  • Participants discuss the effects of capacitor size on circuit behavior, noting that larger capacitors may behave differently due to series inductance.
  • One participant raises a question about the resonant tank acting like a resistor at resonance, while another clarifies that it does not inherently dissipate power and has selectivity.
  • Concerns are raised about the implications of using a parallel tuned circuit with a transistor or FET, as it may lower the Q factor.

Areas of Agreement / Disagreement

Participants express varying levels of understanding and agreement on the roles of components and the behavior of the circuit, indicating that multiple competing views remain. The discussion does not reach a consensus on several technical points.

Contextual Notes

Participants mention various assumptions and calculations related to component values and circuit behavior, but these are not universally agreed upon. There are unresolved questions regarding the definitions and roles of certain resistances and how they relate to the overall circuit performance.

Who May Find This Useful

This discussion may be useful for individuals interested in oscillator circuits, simulation techniques, and the theoretical underpinnings of resonant circuits in electronics.

greg997
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Hi, I've got a few questions about that common base colpitts oscillator. I am trying to simulate it but, I am not sure if the circuit is complete or is it missing anything? I have some formulas but not sure how to use them.I have some assumptions, are they right?

1. Capacitors R3 R4 nad R5 can have any value, but at given frequency must act as short circuit, that means impedance must be small, so the capacitors value must be high. What is the resistance that is considerd short circuit? 1 Ohm? I can't see what I need that C4 for.

2. L resonant Q factor. From formula Q= wL/R. What exactly is that R? Is it like collector resistor in a dc circuit? And when I got Rload , how is it related to R? I've got something called [Total equivalent load resistance across oscillator output at given frequency. I ve got Rload, calculated from output power and peak Ac output.

I have formula Rt= (RdRo)/(RdRo), which does not make sense because the nominator and denominator are the same. Is the Rt= that total equivalent resistance?, then what is Rd and Ro? I've formula for Rd= L/Cr. but now i don't know what is Cr.

3. At what point should I see oscillation? Across the load or transistor? So far I can see only dc voltage equal input voltage. Should I seen pure sinewave?


Appreciate any help and explanation. Those values of resistors and capacitors are random. I just need general answer not calculations. Thanks
 

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I drew this up in a different simulator (LTSpice) but it may work in yours:

[PLAIN]http://dl.dropbox.com/u/4222062/Colpitts%20Oscillator.PNG

Basically, it is the same as yours except the emitter resistor and one of the bias resistors had to be changed.

Output of 27 Volts p-p is available at the collector of the transistor. Oscillation is at about 3.5 MHz.

1. Capacitors R3 R4 nad R5 can have any value, but at given frequency must act as short circuit, that means impedance must be small, so the capacitors value must be high. What is the resistance that is considerd short circuit? 1 Ohm? I can't see what I need that C4 for.

R3, R4 and R5 are resistors, not capacitors, and I don't understand the rest of this paragraph.
Maybe you could have a read of this:
http://en.wikipedia.org/wiki/Capacitors
to understand what capacitors are used for.

Don't forget to ground the main part of your circuit. The rail along the bottom must be grounded or connected to the negative side of the battery for the circuit to work.
 
Last edited by a moderator:
HI, thanks for the replay.
Yeah, That was my mistake with the resitor and capaitors names. I meant capacitors C3 C4 C5. I created your circuit in Multisim and there is sinewave, not a nice pure one but it is there :)
In your case, the impedance of the capacitors is 4.5 Ohm, so I guess that is considerd short circuit. I created my own new circuit and it wroks now. Can you tell how exactly I can see the oscillating frequency, I mean how can I confirm that the oscillation frequency is what it is suposed to be.
And I calculated Load Resistror from Pout= Vout^2/2Rload but the power Pout is twice of what I wanted and Vout Ac is nearly twice then the one used for the formula above. So I got stuck again.

I hope somebody can explain my question in the point 2.

Thank you
 
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To measure the frequency, you need to measure the period first.

Measure the time between two successive peaks on the waveform. Then just take the reciprocal of that time. With my simulator, you just put the cursor on the spot you want to measure and then read it off the bottom of the screen.
You could also measure the time for, say, 10 cycles of output. Then divide the time by 10 to hopefully get better accuracy.

Q= XL/ R where R is the resistance of the coil wire.

Actually, it is also affected by any parallel resistance. This includes the output resistance of the transistor, the load and, in this case, the emitter resistor.

Read about this in any good book about RF tuned circuits. I have an old book by Terman (Electronic and Radio Engineering) that handles this very well, but any good book on this topic should deal with it.

Yes, a few ohms of reactance doesn't matter in circuits where the other reactances are much higher.
 
On a simulator, bigger bypass capacitors will appear to be better.

In real life, capacitors have series inductance and behave like series tuned circuits.

So, bigger capacitors can have a lower series resonant frequency, and above this frequency they behave like inductors.

This also means that if you get the series resonance exactly right, you can have this series resonance giving you perfect bypassing for a very narrow range of frequencies.
 
Hi, thanks for that explanations, that really helps.
One more question. Is that rigth that at resonace the resonant tank acts like resitor due to internal inductor resistance? So it is like collector resistor?
Now, I reading some books about that topic, hope to find what I need.
 
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If the parallel tuned circuit were perfect, at resonance, it would have infinite impedance and its resonance would be only over a very narrow range of frequencies.

Since it is not perfect (because it is loaded by various resistors, including the coil resistance), then it has less impedance than this and it works over a wider range of frequencies.

It really isn't like a resistor. It has selectivity and it doesn't inherently dissipate power.
It can also produce some surprising effects which magnify voltages and currents within the tuned circuit.

You can think of high impedance a being a bit like high resistance, but beware of thinking the two are really anything like each other.

Also, you should be aware that a transistor or a FET should not have a parallel tuned circuit as its load. Both have low output impedances and they lower the Q of a parallel tuned circuit in their outputs.
These should normally be connected to a low impedance tap on the coil or a low impedance winding placed near the main coil.
 

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