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#91 |
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diyAudio Member
Join Date: Nov 2010
Location: The City, SanFrancisco
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Seems like this can be a real fun and entertaining excersize if just not taken too seriously.
Is there any consideration to try and exploit any potential advantages of "newer" available discrete components, which I can only think of the small signal mosfets (Siliconix-Vishay..). Mixing the best characteristics of FETS/BJT/MOSFETs also has some appeal for discrete. Thanks -Antonio |
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#92 |
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diyAudio Member
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#93 |
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diyAudio Member
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Scott - you have the floor/ball..... take it and run. Are you going to do a discrete version of the 627 with us? Or? -RNM
Last edited by RNMarsh; 23rd August 2012 at 05:32 PM. |
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#94 |
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diyAudio Member
Join Date: Nov 2011
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....but did not include in his analysis important one that's been around for ages as discrete design.
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#95 | |
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diyAudio Member
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Quote:
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#96 |
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diyAudio Member
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#97 | |
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diyAudio Member
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Quote:
I think I inherited it and screwed it up a bit This was in the early days. The line of automotive amps didn't sell very well; they were too expensive, and because of the "transverse tunnel cooling" didn't have the large expanse of heatsink beloved of the kids.
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#98 |
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diyAudio Member
Join Date: Nov 2010
Location: The City, SanFrancisco
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Along the lines of SI1029X and or subsequentially larger devices (problem is even when I was using these a few years ago the parts wer becoming obsolete so quick, but at least they were being replaced with newer part numbers).
So I dont know what is readily available today but there seems to be a number of mfgr's and series to speculate from. Hope this helps -Tony |
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#99 | |
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diyAudio Member
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#100 |
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diyAudio Member
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Since virtually all of the likely designs to pour forth are going to want an output buffer, I dredged up and dusted off the attached.
It can be scaled back to lower rails without too much trouble. The bandwidth per se from a 1k source R is about 35MHz. There is the advantage of reduced thermal distortion when used with about a 515 ohm load, since the output devices are equidissipational*, that is, their dissipations roughly track. But when, as we anticipate, this is inside of an overall global loop with plenty of loop gain, the rest of the works will easily correct for dissipation-induced shifts, as the shifts should be fairly slow, and thus the thermal concerns should be minor. The bootstrapping of the input devices raises the input Z, but also requires some lumped C to reduce peaking. Since such C is constant, the distortion at high frequencies at the input is reduced. Short-circuit protection is left as the proverbial exercise to the reader. Brad *the approximate condition for this is that the peak output current into the load at just before onset of clipping is twice the quiescent current. Things are slightly more complicated by the emitter ballasting and the fact that the input devices draw their operating current from the output devices due to the bootstrap arrangement. |
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