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#841 | |
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diyAudio Member
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Quote:
I wish that tankcircuitnoise (and everyone else) would also wander over to here: paralleling film caps with electrolytic caps I haven't had time to get back to it, yet, but I'm still excited about paralleling caps without any conductors in common, so that the total ESL of the paralleled cap/conductor combinations might be reduced in the same (algebraic) way that the total resistance of parallel resistances gets reduced, which I have read (in Ott's latest EMC book) can't properly occur if there is any MUTUAL inductance; ergo my belief that paralleling the conductors as well as the caps might provide a possibly-significant benefit. I started thinking about that for cases where multiple parallel decoupling caps might need to be used across one set of pins (when planes are NOT being used, as is the case for a lot of DIY PCBs) in order to lower both the ESL and the ESR so that the (local) "power supply" impedance seen by the power pins of an amp chip, for example, could be made low-enough, to a high-enough frequency, to provide for good-enough transient response [ f = 1 / ( (π) (risetime) ), I think ]. THEN I realized that MAYBE it would also be a good idea to use multiple parallel copies of the power and ground rail traces, ALL the way from the rectifiers to the load's power pins! i.e. EACH smoothing cap (or each subset of smoothing caps) would have its own rails, all the way from the rectifier bridge (or maybe after the first big cap) to the load. And actually, for low inductance connections, in general, couldn't we just use multiple parallel traces, or, in the case of a board interconnect, a ribbon cable with multiple conducors for each rail and ground? Anyway, I guess those things should be discussed in the thread at the link I gave, rather than here, unless they're applicable here too of course. Cheers, Tom Last edited by gootee; 11th January 2012 at 03:27 AM. |
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#842 |
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diyAudio Member
Join Date: Nov 2010
Location: The City, SanFrancisco
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#843 |
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diyAudio Member
Join Date: Jan 2012
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Or read this appNote from AnalogDevices. The idea of currents taking ALL possible paths at DC, yet becoming more concentrated under the outgoing wire as frequency
increased, was a real eye-opener for me. And while reading a Schaum's Outline book on E&M, to be told coax-cables began to be effective at about 50KHz: surprising. Apparently near 50KHz, the inductance in paths far away from the shield becomes enough to "encourage" return-currents to "choose" the coax-shield. Its all part of minimizing the stored energy, I think. Anyway, after reading this ADI Brokaw AppNote, I began to understand planes, and even to use slits as further "encouraging" of return currents. Just do not route ANY Any any fast signals over slits. http://www.analog.com/static/importe...0828AN_345.pdf |
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#844 | |
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diyAudio Member
Join Date: Oct 2003
Location: osorno , Chile
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Quote:
I've used -ECdesigns'- stepped rectifers concept in both low and high power application with success. It can use 3 or more stepped diodes. I attach one of his diagrams: https://picasaweb.google.com/lh/phot...eat=directlink Of course parts and values can be changed to your specific needs... What do you think? I found it brilliant. Cheers, M.
__________________
Cheapest horn speakers: https://picasaweb.google.com/lh/phot...eat=directlink |
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#845 |
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diyAudio Member
Join Date: Sep 2009
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Hello Gootee,
Relationship is: Bw * Tr = 0.35 Regards. Alain. |
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#846 |
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diyAudio Member
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Interesting. The form that I gave is equivalent to
Bw * Tr = 0.318 (i.e. = 1 / Pi ) I wonder what causes the difference. The equation that I gave came from Henry W. Ott's famous book, "Electromagnetic Compatibility Engineering". I didn't see the derivation and am too old to remember how to re-derive it. |
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#847 |
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diyAudio Member
Join Date: Sep 2009
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#848 | |
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diyAudio Member
Join Date: Nov 2011
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I'll take a ride in this long thread - a really nice one - to add my 2 cent:
Quote:
It seems obvious that anything here should be related to the changes in the output devices voltages (Vce, Vds or Vpk) due to the finite supply admittance - specially regarding the tracks and wire inductances. Transients could have even more impact. Sure, that includes the current return path and eventual decouplers too. These voltage changes would impact the output via the finite impedance of the output devices (early effect, capacitances and the like). Some of this effect is cancelled by negative feedback, but this is also finite. And there's also the possibility of any of these impedances / admittances to be non-linear, adding insult to injury. I was just thinking about a way to measure this. Sure, distortion, spectrum analyzers and stuff. But also there should be a way to provoke the effect. Maybe a good way to test this would be adding series resistors and/or inductors to the PS rails - between reservoir capacitors and rail decouplers and/or between decouplers and output devices - and watching the effect with a test signal. The test signal could be a sinusoidal, where the distortion effects can be more easily measured, or a damped sinusoidal, to get the effect of a transient. But it would tell a lot to watch the rail voltage right before the output device (collector, drain or plate). I'd bet some inductance here would cause a short and deep drop. If driven far enough, this drop would disturb the output device quite a bit. I wouldn't be surprised if some conditions actually saturated the output device, even when the output is far away from the rails. Sadly, I don't have the resources yet to do this test. But, just in case someone luckier has good stuff and time in his/her hands, and wants to figure this out, here goes my suggestion. Best regards all, Emerson |
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#849 | |
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diyAudio Member
Join Date: Jul 2005
Location: D-55629 Schwarzerden
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Quote:
Transformer - Wikipedia, the free encyclopedia and this: http://www.scholar.de/studenten/lern...chaltungen.pdf If I would have this for each transformer and other power supply parts of an certainly amp model so as the individual curvature include clipping/distortion effects of the individual mains socket in the wall, it would be an easy task to intestigate the different effects and reasons for the sonic differences while listening tests by a p-spice simulation. Last edited by tiefbassuebertr; 13th April 2012 at 09:07 PM. |
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#850 | |
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diyAudio Member
Join Date: Nov 2011
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Quote:
What I believe that should be found is the relationship between rails sagging and rising distortion. Surely, the transformer, the mains, etc., all affect sagging in a "long" fashion (>~10ms), by their ability to recharge the reservoir caps. But, in the end, it's just sagging - if the rails drop 1V, the output devices will have 1V less, no matter which part of the supply chain lost this V. So my point of view is that, if some transformer or capacitor is said to be better, my guess is that it reduces sagging, so output devices suffer less. Or, from another angle: whatever good the cap/transformer/rectifier/mains combination is, we can make it 1 ohm worse, or 1mH worse, or both, and already have a clue of the mechanism Bob is searching. If you're simulating, you can also make it 1 ohm or 1mH better... With the complete models, then we can tell how much. Best regards, Emerson |
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