Charles Hansen come in please

Status
Not open for further replies.
i fear the moderators don´t like these kind of words....

do we wanna go back to feedback (or nonfeedback) now?

the circuits from Charles link looks not really low parts count and simple to me - compared to Nelsons preamp schematics.
 
till said:
the circuits from Charles link looks not really low parts count and simple to me - compared to Nelsons preamp schematics.
From what I understood, this is the circuit of the Ayre v-3, and this should be a power amp, not a preamp (but you can drive it from a CDP).
However, it is not clear to me how Q7 / Q8 are working. The gate is somehow attached between the output and rail - cascode? Sorry for the silly question, but I'm a very beginner....:bawling:

Cheers, Tino
 
Charles Hansen said:
Let's look at your example of a single cathode follower and think about what's going on. For the moment, let's tie the grid to the cathode but leave the heater and power supply connected. The tube is now acting like a diode (we can pretty much ignore the grid for now).

Ok.

There is a stream of electrons heading from the cathode to the plate, and the current flow is limited by the combination of the cathode resistor and what is called the plate resistance. There current is expressed in amperes, which is expressed in Coulombs per second (a Coulomb is 6.022 x10^23, or Avagadro's number of electrons), so even with a very small current there is a large number of electrons flowing in the vacuum.

Ok.

There is even a way to calculate the velocity of the electrons. Their kinetic energy is expressed in electron-volts, and is a function of the voltage impressed upon the tube. I'm not a tube guy and I'm too lazy to look up the proper constants, but suffice to say that both the effective potential (voltage) and electron velocity will vary as a function of the distance between cathode and plate, and that there is a finite transit time for the electrons' flight.

Ok.

Into this nice little picture we now apply a voltage to the grid that is negative relative to the cathode.

Aren't you forgetting something? Better apply a load resistor too if you expect to get any output from this thing.

So some electrons go marching up the wires to end up on the grid itself. Relatively speaking, it doesn't take a whole lot of them, as all we have to do is charge up a small capacitor. Using the formula Q = CV (where Q is again expressed in Coulombs), let's assume 1 volt applied to the grid and an interelectrode capacitance of 10 pF (about the right order of magnitude for a small signal tube). Then we will stuff about six-quadrillion electrons up onto the grid.

Ok.

This doesn't happen instantaneously, of course, but instead as the exponential charging of the capacitance. Since this is a tube circuit, let's assume this circuit is being driven by a source impedance of 500 ohms along with another 500 ohms of grid stopper resistance for a total of 1000 ohms. (We know the grid stopper makes the circuit sound better, although we're not exactly sure why....) This gives a time constant of 10 nS, which means it will charge to 1/e = 63% of the final voltage (1 volt) in that time. After three time constants, it will have charged up to 95% of the final voltage. So right off the bat we have created a low-pass filter with a -3 dB point of around 17 MHz.

Aren't you forgetting something? Like the load resistor again? The cathode isn't connected to ground anymore, remember? So why are you calcultaing the time constant based solely on source impedance?

Looking at the equivalent circuit for a triode, configured as a simple cathode follower with a load resistor, it appears to me that the gate to cathode capacitance's path to ground is through the parallel combination of the load resistor, plate resistance and the plate to cathode capacitance.

Back inside the tube, now. As the electrons move onto the grid they radiate an EM field that propagates in all directions at the speed of light. It starts to get a little messy now, as we not only consider the action of this field on the electrons leaving the cathode, but also the electrons already in transit. The electrons already past the grid will experience a slight acceleration and those not yet to the grid will experience a decceleration. This causes some interesting things to happen and is the basis for the operation of things like klystrons and traveling-wave tubes.

Yeah-yeah, sure-sure.

If we ignore this mess and focus only on the steady state (not a bad approximation for an audio amplifier), we will find that the beam current has changed. This change in beam current creates a voltage drop across the cathode resistor, and hence the cathode voltage also changes.

Ah, ok. Now the load resistor appears.

Now the cathode voltage is changed by number of electrons present there, and these electrons have to charge up any capacitance between the cathode and other electrodes, including the grid, plate, and heater.

Wait a minute, you just said that the cathode voltage changed because of the voltage drop across the resistor due to the current flowing through it. Now you're saying that the cathode voltage changed because of the number of electrons there.

Which is it? Did it change because of the voltage drop across the resistor or did it change because there are more electrons on the grid?

So this change doesn't happen instantaneously either, but instead as another exponential function as those capacitances are charged through the cathode resistor.

Yet below you say it does change essentially instantaneously. Which is it? Does it change essentially instantaneously or not?

At this point we have at least 3 distinct mechanisms contributing to the delay between the input signal and the output signal:

- Charging time of the grid capacitance
- Propagation delay of the field from the grid
- Charging time of the cathode capacitance

Not to mention the resistances that those capacitances are charging through.

But please note that as the cathode (output node) itself changes potential ("following" the grid), that the beam current changes essentially instantaneously, with only propagation delay of the field from the cathode having any real effect.

How can it change any more instantaneously than the voltage across the cathode resistor which you just said above doesn't change instantaneously?

The current through the tube is a function of the voltage voltage between the grid and the cathode. Since the grid voltage is established by the input signal and the cathode voltage is established by the cathode resistor, and since you say the voltage across the cathode resistor doesn't change instantaneously, I fail to see how the current through the tube can change instantaneously in response to the voltage on the grid.

The speed of light in a vacuum (ain't tubes great?!) is 3 x 10^8 m/S, so assuming a cathode-grid spacing of 1 mm (about the right order of magnitude for a small signal tube) the delay is around 3 pS, which corresponds to a frequency of around 300 GHz.

If that were the case, then we would also have to expect the tube itself to have a bandwidth on the order of 300 GHz.

I think you need to go back and think this through again.

se

An externally hosted image should be here but it was not working when we last tested it.
 
zinsula said:

From what I understood, this is the circuit of the Ayre v-3, and this should be a power amp, not a preamp (but you can drive it from a CDP).
However, it is not clear to me how Q7 / Q8 are working. The gate is somehow attached between the output and rail - cascode? Sorry for the silly question, but I'm a very beginner....:bawling:

Cheers, Tino

I'm no expert myself, but the gates are at AC ground and the sources are driven by Q1 and Q2. Q7/8 drains drive the output stage. There's a symmetrical antiphase version at Q9 and Q10, but driven by the other side of the input diff amps. It sure looks like a relatively straightforward grounded gate stage.

Charles, you're heartily invited to tell me I'm full of it and explain it properly.
 
If that were the case, then we would also have to expect the tube itself to have a bandwidth on the order of 300 GHz.

Rather than chew through it line by line, I was going to just go home this evening and stick some scope probes on my preamp to look at the actual signal transit time through the CF. But that would be cheating, wouldn't it?
 
Hi,

Yeah it would. Go ahead. Cheat.

The only thing you'd probably learn from that is that the discharge time of a coupling cap is higher than the transfer time of electrons in a vacuum.

If that were the case, then we would also have to expect the tube itself to have a bandwidth on the order of 300 GHz.

You would if it weren't for the inevitable interelectrode capacitances which would require trickery_it exists_ to neutralise.

I think you need to go back and think this through again.

I agree, you are both talking about different things here.

Cheers,😉
 
From what I understand, the transit time and bandwidth of a box of gain are unrelated. In a reductio ad absurdem, you could have an amp with an infinite bandwidth, but which could have a delay between input and output of years. Put in a narrow pulse, wait a year, and an identical pulse comes out without spread.

The philosophical (as opposed to pragmatic) arguments I see against the use of loop feedback are based on its retrospective nature. I honestly don't know offhand how retrospective a CF's feedback is, so looking at front-to-back time will give me a measure of that. Since, as you point out, one of the input ports is connected directly to the output, much in the manner of an opamp connected as a unity-gain buffer (hard connection between output and inverting input), the transit time will give me an empirical notion as to the relative signal delay between the ports.

So... do the FETs I was talking about before work the way I was speculating? I'm trying to learn something about transistor amps and it's always nice to get it right from the horse's mouth, as it were.
 
SY said:
From what I understand, the transit time and bandwidth of a box of gain are unrelated.

Yeah, I was thinking in terms of feedback which in hindsight isn't a bandwidth issue.

If there were no delay between the input signal and the feedback signal, then the feedback signal would never be in phase with the signal and the feedback would never become positive.

In any case, I don't see how the feeback could possibly be delayed by only a few picoseconds as Charles claims unless there were no parasitic capacitance anywhere in the circuit.

se
 
V3proto

Charles,

I have quite the same thinking, but rather different.
Can you call this X-amp? No ground involved in speaker outputs.

My idea is like this, please comment.

The front end is still folded cascode, driving half power amp, resulting in X amp like your V3proto. But I wanted to use only single differential, so dont use Q2-Q4, and replace Q8 and Q10 with CCS. Which is better, replacing Q8-Q10 with CCS or plain resistor (or bootstrap maybe?) if I wanted single differential like I told you above?
 

Attachments

Maybe there is some "mechanism" of delay involved in audio amplifier+feedback path. I remember Nelson Pass said something about "Hall of mirror" effect, if the gain stages in audio power amp is too long. It makes the feedback less effective. Is this caused by time or capacitance delay, maybe inherent in every transistor?
 
Hi,

Well, if your circuit were infinitely small...

Eh, eh, eh....That wouldn't work either...no matter how small it is there will allways have to be a distance between input and output.
To bridge a distance takes? Time.
To charge and discharge a capacitance takes times, to charge a space takes time....even in a vacuum.
To make one triode different from another takes a distance between the elements...and so on.

Just that I don't believe the time involved in the cases we've been talking about here is on the order of a few picoseconds as Charles has claimed.

You still have that stopwatch?:devilr:

Seriously, I think Charles was talking from an ideal model POV. Not necessarily a real situation.
Picoseconds...that's a pretty short distance in time, isn't it?:bigeyes:

Cheers,😉

P.S. Slowly reaching a state of homeostasis....ZZZZzzzzzzzzz.
 
Status
Not open for further replies.