Zero Feedback Impedance Amplifiers

Footnote 1:
I'm left confused because I thought I only needed four more windings in total, two more for the primary and two more for the secondary; a total of 12 windings. Also I was / am assuming the dual-bobbin standard configuration. Across two bobbins, four extra windings would only amount to one extra bi-filar section needed per bobbin.
I will need to do a proper winding calculation - the aim is to have the primaries always tightly coupled in bi- or quad-filar grouping. In a dual chamber bobbin of an EI-120 core winding a hex-filar is going to be very-fiddly. Winding for a C-core might be a bit easier as the bobbins are longer.
I will have to do the proper calcs to confirm.
 
That should work, I also have a couple of 10k CT: 600R Edcors that I intend to try as step up/phase splitters.
The 25-70Hz range should be quite forgiving for cheap transformers.
Nice.
As an alternative to get properly balanced mains transformers to use in reverse as input for bass below 100Hz then one can use this type of Flat Pack transformer:
https://www.mouser.fi/ProductDetail/Triad-Magnetics/FP24-1000?qs=Yx4IQMNd5u5fz6lHd7mh8A==
This has the advantage of filtering HF above c. 1kHz - as the side-by-side chambers don't couple the higher frequencies.
 
I will need to do a proper winding calculation -
... okay @charliemb , some notebook doodling later:
To get 3:1 I had in mind to start with 2:1 and adds some more turns on the primary... not sure if this is ideal as the output resistance is almost the same as with 2:1 config.
EI-120 dual chamber has 25mm x 15mm winding aperture per side; I am assuming however for practicalities one is only going to get 12 layers in because of bulging across the windings.
Currently that gives 12 layers of quad-filar windings at 6 turns per layer, which is 72 turns per wire per side.
Reducing this to 10 layers of quad-filar then 2 layers of bifilar as a separate section reduces the quad-filar wires to 60 turns and adds 24 turns bi-filar per side.

P+
24 |||
24 |||
60 ||| 60
60 ||| 60
GND
60 ||| 60
60 ||| 60
24 |||
24 |||
P-

Cross couple the two secondary sides so that each series section winding is made from one winding from each chamber as with 2:1 setup.

?
 
... okay @charliemb , some notebook doodling later:
Now you are making me think!
...I'll be back.

To get 3:1 I had in mind to start with 2:1 and adds some more turns on the primary... not sure if this is ideal as the output resistance is almost the same as with 2:1 config.
EI-120 dual chamber has 25mm x 15mm winding aperture per side; I am assuming however for practicalities one is only going to get 12 layers in because of bulging across the windings.
Currently that gives 12 layers of quad-filar windings at 6 turns per layer, which is 72 turns per wire per side.
Reducing this to 10 layers of quad-filar then 2 layers of bifilar as a separate section reduces the quad-filar wires to 60 turns and adds 24 turns bi-filar per side.
In the meantime, I understand or assume:
  • "side" means one side of the dual-chamber bobbin;
  • "aperture" means the entire volumetric space inside each side, wherein the aperture has a width of 25mm and enough room for layers of 15mm;
  • "layer" means one row of windings per side of the bobbin wherein the quad-filar section yields 6 turns per layer and wherein the bi-filar section yields 12 turns per layer;
  • sections comprise layers of windings of the full width of each aperture, and there are only two sections per side, one section of quad-filer layers (10) and a second section of bi-filer layers (2) wound directly on top (or underneath) of the quad-filar section;
  • all bi-filar windings remain on the primary side, four separate coils, and no new coils are added on the secondary;
    • the new coils can't be placed in parallel on any of the secondary coils because the EMFs don't match with the EMFs generated by the 60 turn coils (as 24 != 60);
  • The four 60-turn secondaries are connected 2:1, meaning two in parallel placed in series with the other two in parallel, and yes the paralleled coils can and should be cross coupled across bobbins.
Again I will think and get back.

Thanks
 
...I'll be back.
Dada dum de dum!
In the meantime, I understand or assume:
Yes, all correct.

I placed the additional bi-filar windings on the outside as that makes the DC resistance of the secondaries slightly smaller (maybe 5%?), in addition to the decrease from the reduction in the number of turns, compared to having the bi-filar layers first.

General note: Because of the use of a dual chamber bobbin, all winding sections have to be in multiples of 2 layers as the start and stop have to be on the outside.
 
but I'm curious what the reason would be for partially hand winding the output transformer?
The line-driver and power-stage output transformers are completly wound by hand by preference - from experience commercial machine winding bi-filar and quad-filar is not capable of putting down the layers without crossovers in the winding process.

In my case I use my lathe to hold the bobbin on a plate and hand crank the spindle to turn, see pic.

zeus-output-tx-75w-bifilar-pri&sec-single-chamber-myford-lathe-3-800.jpg
 
Nope, BJT transistors by themselves are not more suitable.
I use a Triode-BJT hybrid follower in some of my variations, for example line-drivers as can be seen in the pics in my previous post:
https://www.diyaudio.com/community/threads/zero-feedback-impedance-amplifiers.42259/post-7899562

[but] Not needed in my topology...
Susan, if I may? Something like this Triode-PNP hybrid follower? The distortion depends mostly on triode. The simulation flatters maybe, but still. . Output is 'low enough' for a transformer.
Impedance is fairly constant. [Made with 18042 as a test project for ETF'23; requirement was loading to a 600Ω output]. ECC82 is slightly different. ECC83 is great too. Just compare in vivo.
I am currently using such a stage without transformer : as a buffer after my 50k potmeter. The impulse and low level field presentation are astonishing of this hybrid. The input is self-biassing: the base current, ! Every small change in the coupling cap can be appreciated.
 

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Something like this Triode-PNP hybrid follower?
Nope.

Fine to see your circuit simulations, but it is not my transformer/follower/transformer topology - see schematic and pic.
Tube is 7N7, Loktal version of 6SN7, BJT is 2SC5200.
Heaters powered by a PTN78060WAD non-Isolated DC/DC Converter with slow-start circuit.
B+ is +24V from a separate AC/DC supply.
Input-transformer is Hammond 124B, output-transformer is EI-96 quad-filar wound 0.8mm magnet-wire.

2021-susan-triode-bipolar-hybrid-line-amplifier-sim-schematic-1.png

Schematic of Bipolar-Triode Hybrid line-driver​

susan-hybrid-triode-bipolar-line-driver-inside-view-1-sharpen-Standard.jpg

Inside view of the Bipolar-Triode Hybrid line-driver, in daily use as part of our 5.1 setup.​

susan-hybrid-triode-bipolar-line-driver-on-workbench-1-DeNoiseAI-denoise.jpg

Rear view of the Bipolar-Triode Hybrid line-driver, in daily use as part of our 5.1 setup.​
 
Nice balanced base-current concept. Does it require matched combo's? . . .
Then - Just an old thought: if the base current would be different, then on an ECC82 (version) , a deliberate slight imbalance of the two heater sections would be able to balance that again (Wireless World tip from the sixties).
 
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... a deliberate slight imbalance of the two heater sections would be able to balance that again...
Thanks.

Yes, I am trying out some ECC99s with this in mind for the power stage.
https://www.jj-electronic.com/en/ecc99
I suspect however this may affect the transfer curves and thus the even-harmonics; more testing (and time to do testing) needed.

This is my current test-setup with a 7N7...

susan-breadboard-triode-bipolar-hybrid-test-1-sharpen-Softness.jpg
 
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Can SITs be made to work in the power stage?
Yes, but one would need to bias the SITs as an additional circuit; so one then needs a matched pair and a third one to temp/co track the bias - as I do in my standard MOSFET configuration. If you have a stash, then great. Not sure where to buy any in sensible numbers e.g. 30+ to get matched pairs?
I use Depletion Mode devices that auto-bias through the DC resistance of the windings, makes for simplicity and the input transformer is hard connected to the 0V rail (so one less potential source of noise/distortion).
 
Dada dum de dum!
I'm back. Regarding the 3:1 ponder and the prototype proposed here:
... okay @charliemb , some notebook doodling later:
To get 3:1 I had in mind to start with 2:1 and adds some more turns on the primary... not sure if this is ideal as the output resistance is almost the same as with 2:1 config.
EI-120 dual chamber has 25mm x 15mm winding aperture per side; I am assuming however for practicalities one is only going to get 12 layers in because of bulging across the windings.
Currently that gives 12 layers of quad-filar windings at 6 turns per layer, which is 72 turns per wire per side.
Reducing this to 10 layers of quad-filar then 2 layers of bifilar as a separate section reduces the quad-filar wires to 60 turns and adds 24 turns bi-filar per side.

P+
24 |||
24 |||
60 ||| 60
60 ||| 60
GND
60 ||| 60
60 ||| 60
24 |||
24 |||
P-

Cross couple the two secondary sides so that each series section winding is made from one winding from each chamber as with 2:1 setup.

?
Here is my analysis with estimates.
4:1 Standard
Sowter 9840 OPT
2:1 Standard
Sowter 9840 OPT
3:1 Hexa-filar wound 3:1 Extra primary windings,
Standard 2:1 output wiring.
As proposed in the above post.
Total output impedance 0.257 Ω 1.03 Ω 0.456 Ω 0.62 Ω
Damping factor 31.2 (8Ω)

15.6 (4Ω)
7.8 (8Ω)

3.9 (4Ω)
17.54 (8Ω)

8.77 (4Ω)
12.82 (8Ω)

6.41 (4Ω)
Average power output (best-case for 48 V DC supply) 33.8 Watts into 8Ω

63.6 Watts into 4Ω
113.1 Watts into 8Ω

182.4 into 4Ω
57.3 Watts into 8Ω

103.1 Watts into 4Ω
63.2 Watts into 8Ω

110 Watts into 4Ω
Turns ratio 4:1 2:1 3:1 2.8:1
Impedance ratio 16:1 4:1 9:1 7.84:1
Secondary winding configuration Four in parallel,
none in series
Two in parallel,
two of those in series
Three in parallel,
two of those in series
Like 2:1, Two in parallel,
two of those in series
Relative distortion levels Lowest Higher In between, probablyIn between, probably
Bias current commentary for a given idle dissipation Tends to stay in Class A the longest, but high rail voltage requirements limit bias current.

Potentially not the best compromise but offers the best damping factor.
Tends to move into Class A/B the quickest due to highest primary currents. Could tend to stay in class A comparably to 4:1 after increasing the bias current and lowering the rail voltage accordingly for the same power output.
- Or, a higher power output can be chosen and move into class AB a little sooner.
- Potentially closer to optimal but can only be considered if the damping factor is acceptable.
Ditto, as with 3:1.


For the hexa-filar wound case, an assumption was made that more coils compensates for fewer turns per coil in order to fit within an EI-120. That is, the primary-side resistance is the same as for a Sowter 2940.
 
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One thing to note on distortion (from measurements I did a long time ago with my HP8903B Audio Analyser), that after exiting Class A in PP the distortion flatlined until the primary-followers approach the power-rail.
Yes. That flattening has always intrigued me. The flattening surely was after exiting Class A. Just now I became curious about how far after exiting Class A and so I looked up some of my previous work from back in those days. It shows that a Zeus 2:1 idling at 750 ma exits Class A at 4.68 volts (1.37 Watts into 8Ω). That would be just past half way toward flatlining, right in the middle of the above graph.

If indeed the crossover point happens in the middle of the graph, then the implication is that crossover events are relatively insignificant in a Zeus. Audibly, I can confirm by ear that lowering the bias current is hardly noticeable. (I still crank it though.)

What hypotheses have floated which could explain the flattening?

Here's one: The flattening occurs deep into the square-law curve of the MOSFETs. Being far into their square-law curves, a MOSFET pair from the same tube and with similar idle bias traits (where you selected them) tends to match where the flattening begins. Either the curves become linear, and some MOSFETs are known to go nearly linear (early HEXFETs), or the curves become true parabolas and the difference of squares is linear anyway. Hence, at that point, something close to no new distortion is added. And after that point, maybe it is only proportional distortion added by the transformers, remaining at 1%.
 
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I purchased my Sowters and have never wound a transformer.
When the 4:1 is wound starting from the left with wires
► 1 2 3 4 and moving toward the right ►, when reaching and end of the bobbin the four wires now have to go toward the left. When moving toward the left, do the wires remain in the same orientation
◄ 1 2 3 4 or do they flip as follows
◄ 4 3 2 1 ?