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#11 |
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diyAudio Member
Join Date: Sep 2010
Location: East Tennessee
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Kinda looks like the input of a bipolar IC, but the current mirror is only one sided, one side of the mirror is a constant DC voltage, the other swings between the collectors, errr collector and plate.
The second design sets the VBE of both output current sources, the 1k desensitizes the design to VBE/IC variation, so now you loose the mirror to just current sources and improved linearity and differential output. You could make one of the 1k's a pot to balance the stage. In IC's we would use a NPN mirror on the bottom to run the diff pair off of the same bias resister. Again you can use a mismatch in the emitter resisters to set the current ratio. A pot would make it adjustable.. Quite a hybrid circuit. The MPS trans are only good to 300V with a beta of 20-40
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SO many tubes, SO little time!!! |
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#12 | |
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diyAudio Member
Join Date: Jul 2005
Location: South Florida
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Quote:
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Too much power is almost enough! Turn it up till it explodes - then back up just a little. |
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#13 |
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diyAudio Member
Join Date: Feb 2004
Location: Silicon Valley
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Roline - the typical gain of the MPSW92 is much higher - on the order of 100 or so, and of course I can select high gain units. The tubes at the bottom will help keep the top transistors from seeing their max voltage. 10-20k in series with each collector would also help.
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#14 |
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diyAudio Member
Join Date: Dec 2001
Location: Hickory, NC
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Something like this for a complementary mirror load. Q1 and Q2 are P channel Mosfets. R1 and R2 around a Meg-Ohm. Although this is the more obvious way of making one. J.L. Hood's version looked more clever as I recall. To the point that I couldn't figure it out. I don't think it had any control resistors down to the drains.
Maybe it had extra P-chan source followers driving R1 and R2, so as to not load down the outputs. Just guessing. Hmmm, or how about a floating NPN cascode set below Q1 and Q2. Current into their bases from Q1,Q2 drains would determine the output currents (xBeta) and the control voltages for R1,R2 could come from the base voltages. Wild speculation.
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Ohms Law V = I R Last edited by smoking-amp; 2nd January 2011 at 02:02 AM. |
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#15 |
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diyAudio Member
Join Date: Dec 2001
Location: Hickory, NC
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Well, I don't know how J.L.H. did it, but I've figured out how to do it without any loading on the outputs now. Call it the Cas-complement mirror. Q1 thru Q4 are P channel Mosfets. Q3 and Q4 can be low voltage types. R1 and R2 around a 100K Ohm say still. Q3 and Q4 act as floating cascodes in the downward direction, and as source followers in the upward direction. A class act.
edit: Hmmm,, Errr... except one could also call Q3 and Q4 low voltage zeners. Guess they aren't doing much useful. Nevermind.
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Ohms Law V = I R Last edited by smoking-amp; 2nd January 2011 at 03:00 AM. |
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#16 |
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diyAudio Member
Join Date: Jan 2008
Location: Eureka, CA
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How about the differerntial gyrator?
Another kind of hybrid I have an improved version but the basic concept is the same. Cheers, Michael Last edited by Michael Koster; 2nd January 2011 at 03:29 AM. |
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#17 |
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diyAudio Member
Join Date: Sep 2010
Location: East Tennessee
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Just for fun, spud re-hashed.... Tried to keep as much of the original design with current biasing.
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SO many tubes, SO little time!!! |
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#18 |
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diyAudio Member
Join Date: Dec 2001
Location: Hickory, NC
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Yeah, Michaels got the differential load in fit form. I still would like to find that J.L.H. version someday. (was an old W. W. article for a SS amp)
Spud Re-Hashed! Nice scaleability of current thru-out! Laser trimmed? Was it Zilog that did a CPU chip once that had an IC socket on the back? Two compactron sockets topside could be tight. Brings to mind an interesting chassis design. Put all the parts in a long rectangular case, similar to an IC DIP shape, with a bunch of shiny "lead wires" sticking out along the bottom edges for springy support, and the compactrons plugged into the topside. Toroid OT inside out of sight. Power supply from an umbilical. A small notch in one end of the chassis for orientation. Epoxy black finish. A new meaning to "integrated amp".
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Ohms Law V = I R Last edited by smoking-amp; 2nd January 2011 at 04:12 PM. |
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#19 |
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diyAudio Member
Join Date: Dec 2001
Location: Hickory, NC
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Looking at Michael's Differential Gyrator schematic(s) using caps in the cross coupling controls gives me an idea on how to eliminate the residual V sense resistor loading (for AC) on the tube outputs. Since the current drawn by those V sense resistors is predictable, one could use Hawksford's cascode compensation technique to remove the same currents from the Mosfet outputs.
Need some resistance in series with the D1,D2 Zeners, and a small cap (like pF) from R9 and R12 top ends (improved version posted) (or could just use another set of sense resistors) to the same side Mosfet sources. Idea is to subtract out from the Mosfet current (at it's source) the same tiny AC current as drawn by the sense resistors, making them transparent effectively.
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Ohms Law V = I R Last edited by smoking-amp; 2nd January 2011 at 04:38 PM. |
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#20 |
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diyAudio Member
Join Date: Dec 2001
Location: Hickory, NC
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In simplified form, something like this:
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Ohms Law V = I R |
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