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#1 |
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diyAudio Member
Join Date: Jul 2005
Location: D-55629 Schwarzerden
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last weekend I have heard two different power amplifiers by direct comparsion:
1) Pass "X 600" vs. 2) Yamaha "MX 10.000" (MX10000, MX-10000) I was surpriced about the low sonic differences between this two devices and I guess, that the HCA technology is also a good solution, especially if the loss power must be lower by the same output power. Are there HCA diy projects respective other commercial amplifier brands, where is HCA technology inside? Thanks for your advices. Short form HCA describtion you find here: http://wired4sound.net.au/amplifiers...aha_mx_800.htm At the next time I will try to create any simulating results by this amplifier technology Last edited by tiefbassuebertr; 30th September 2009 at 11:52 AM. |
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#2 |
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diyAudio Member
Join Date: Nov 2007
Location: Dallas
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Pair of Schottky non-linear resistances spanned between two offset followers
gives the following push and pull currents into the load: I've never been sure if this behavior was Class A? or Class AB? Maybe its your Hyperbolic thing? |
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#3 |
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diyAudio Member
Join Date: Oct 2008
Location: Vancouver
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Is there a schematic of the OPS?
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#4 |
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diyAudio Member
Join Date: Nov 2004
Location: Suomi, Finland
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Damnit, MX-1000 and MX-2000 (amps with the same feature) service manuals are missing the pages that have schematics!
Anyone have these? |
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#5 |
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diyAudio Member
Join Date: Nov 2007
Location: Dallas
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cbdb>Is there a schematic of the OPS?
Yes. This circuit I am about to show you is an older one, created the above plot. Certainly not the simplest, nor best way I could have drawn for you today. Magic is simply two independent single ended class A amplifiers, any type will do. Offset one amplifier to track one emitter drop above the desired output voltage. Offset the other one to track one emitter drop below the desired output voltage. A quiescent current is set by resistors spanning the gap between these two offsets. If that resistance is linearly resistive, then only linear class A crossing can be the result... Power wasted at quiescent is exactly the same as at full output swing. But if that resistance rides on the curve of a non-linear diode.... You can shape it. The Quiescent current can be far less than full output swing. But still no transistor is ever turning off. This is my own circuit, nothing to do with Yamaha's. And possibly irrelevant. We still at this point know nothing about "Hyperbolic" to guess what that means? But the Yamaha advertised description (so far) fits how mine behaves to a tee. Is Yamaha using the same trick, or I've spun completely off a different tangent??? Last edited by kenpeter; 30th September 2009 at 07:16 PM. |
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#6 |
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diyAudio Member
Join Date: Oct 2008
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Hi
I think that you can find both service manuals and schematics at Jan Dupont’s website ACD http://www.audio-circuit.dk/ BTW look at patent US4803441 Cheers |
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#7 |
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diyAudio Member
Join Date: Nov 2007
Location: Dallas
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Darn, and I thought MY way (with a big Schottky) overcomplicated.
Yamaha looks like an analog computer based upon log nonlinearity of bipolar transistors??? How they keep that from becoming temperature dependent? A Schottky on the other hand dissipates almost nothing in this application compared to the capability of its TO220 package... But I think we are talking the same end result, as far as current go. |
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#8 |
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The one and only
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All these efforts (going all the way back to the Threshold
dynamic bias patent) exploit some non-linear function to keep the output stage in forward bias. The presumption is that this non-linearity is better than the one in the output stage devices.
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#9 |
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diyAudio Member
Join Date: Feb 2001
Location: illinois
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this all sounds like barry thornton's "hypersonic class a" from those old (and nice i thought SAE amps). i think he used schottkys in the output stage also.
hmmm ... maybe i shoulda kept quiet, i might be dating myself again ... mlloyd1 |
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#10 |
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diyAudio Member
Join Date: Nov 2007
Location: Dallas
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Its far easier to match curve of an identical two terminal diode to compliment
the same on the flip side... Than trying to match up swervie-curvies of an NPN to PNP, especially if those same devices are also the ones dissipating the big power... Many of the purpose built complimentary pairs have lots of emitters with series resistance, too linear. Just build in some error correction, and let them be as linear as they wanna be, why fight it? The Schottky can't drop more than .3 forward volts, so its largely out of the power dissipation business at any realistic Class A current. But it gives back the curves we need to achieve this A-AB-hyperbolic crossing or whatever it is... |
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