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#11 | |
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diyAudio Member
Join Date: May 2002
Location: Switzerland
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Quote:
2.) Maybe, but keep in mind that there always people on this forum who are deliberately or carelessly p****ing the old experienced guys off. And JC might be more susceptible to this than NP. But that should not keep us from being grateful that there are exeperienced people sharing their views and thoughts with us. Regards Charles |
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#12 | ||
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diyAudio Member
Join Date: Jan 2004
Location: away
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Quote:
While in theory, the two speakers have to be absolutely identical to guarantee soundstage, we do tend to adapt to the nonconformities as we listen. Quote:
Cheers, John |
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#13 | |
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diyAudio Member
Join Date: May 2005
Location: Pretoria, South Africa
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#14 |
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diyAudio Member
Join Date: Aug 2001
Location: Cape Town, South Africa
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When I built a MOSFET amplifier (ETI5000) in my first year at tech back in 1985, I could not at first figure out why the overload protectors on those B&W speakers kept tripping, even at moderate levels. A few years later I discovered a 4MHz oscillation present at the output of these amps. I resolved this by installing drain-gate capacitors (IIRC) on those output transistors.
Now, I'm thinking: how many other amps out there employ electronics that can interact with out-of-band signals or loads? We mostly limit amplifier bandwidth by installing an input filter, and neglect what happens at the output side. We convince ourselves by proving that significant cable effects do not exist within the audio band. But what if cables do indeed induce (certain) amplifiers to become unstable outside the audio band, or admit RF signals? And what if these effects manifest themselves as reduced fidelity of the audio signal?
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Shaun Onverwacht |||||||||| DON'T PANIC |||||||||| |
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#15 | |
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diyAudio Member
Join Date: May 2006
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Quote:
The Cobra cables had very high capacitance, trying to get to a low characteristic impedance I guess. The PL amps would go unstable from the lowered output pole frequency formed with the high capacitance. The HF oscillation would fry the amplifier because the bipolar output transistors in the PL couldn't turn off as fast as they could turn on, and so caused massive current to go through the transistors (same would happen if you drove the amps full scale at very high frequencies). The problem with trying to use cables matching the impedance of loudspeakers is that speakers are only *nominally* 8 ohms (or whatever). It's not unusual to have a 10:1 difference in speaker impedance over the audio range. At even higher frequencies, cone or dome speakers usually have a very high inductive impedance, so all the amplifier sees is the speaker capacitance that is in parallel with that high impedance. The benefits of using cables matching the speaker impedance are doubtful (IMHO). |
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#16 |
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diyAudio Member
Join Date: May 2005
Location: Pretoria, South Africa
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Again, I am surprised.
I was of the opinion that one of the basic requirements of an amplifier design was that it should be stable with normal operating output loads - i.e. including whatever cable capacitances and load variations would normally be encountered. In my own designs I was never quite comfortable unless they were stable even with open load (perhaps a little vanity ... who knows). I mostly seem to be able to achieve this. Coming to the point: Yes, obviously the sort of thing mentioned in the previous 2 posts (Bvaslo and Shaun) would cause havoc, and should not occur. Nowadays the easy way out of that sort of problem is a small series inductor in the output circuit.* (One never had those problems with tube designs because there was always a large series inductance - the OPT leakage reactance.) So, I would risk saying if an amplifier is prone to that kind of instability - redesign! Perhaps bold words, but I am an amplifier designer and cannot agree that such a state of affairs should necessarily exist. If one is the owner of such an amplifier without technical expertise to rectify the situation, hopefully a knowledgable person could be found to assist without having to throw the amp out. (A signal generator and scope would be required for a proper analysis.) _____________________________ *This was the subject of a drawn-out discussion elsewhere. |
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#17 | |
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diyAudio Member
Join Date: Aug 2001
Location: Cape Town, South Africa
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Quote:
What is worrying, though, is that mostly these effects are reported by users of high-end equipment(!)... of which the expectation is that it is amongst the best in the world (the equipment, that is
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Shaun Onverwacht |||||||||| DON'T PANIC |||||||||| |
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#18 | |||||
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diyAudio Member
Join Date: Jan 2004
Location: away
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Quote:
If one were to contrast two ten foot cables, the first 1nSec per foot and 4 ohm Z, vs another at 2nSec per foot and 100 ohm Z, both feeding a 4 ohm load, what would the step response be? For cable 1, the load voltage and current are that of the intended signal, exactly 10 nanoseconds after the amp produces it. For cable 2, 20 nano out (remember, it's 50%c), it is 1/25th of the final signal. Reflections reach the load every subsequent 40 nanoseconds, each reflection that hits the load increases the volt/current at the load 1/25th of the difference between the intended signal, and that currently at the load. That is a discrete decaying exponential. And it is double the response time of the lumped element analysis of the cable inductance would indicate. And, the first cable has ZERO response time (other than the transit time). So clearly there is a marked electrical difference between a zip cord, and a matched cable. Audible? Don't know, suspect maybe, nobody's proven such. Quote:
Plug em in, play music, sit in the sweetspot. Would we know if the sweetspot shifted a really small amount due to the diff? I wouldn't, as I've no head vice.. The point being, we adapt to this small shift by moving our head, even 100 mils... Go three way now. Same deal?? Not exactly. The sweetspot for the midrange may not be the same as that of the tweeters. Sibilance may be offset w/r to main vocals, especially if the drivers weren't matched. Very good speaker vendors would be concerned with that problem..I know I would. I've made my own systems where the tweeter cap tolerance did shift sibilance in that way. The equivalent amplitude or timing shift needed to make that shift in sibilance? The numbers are small enough to boggle the mind of any intelligent person. 2 to 5 uSec interchannel? Tenth dB??? Ridiculous numbers..but the equations are robust..and I cannot rule out the possibility of some cable effect causing problems at that level. Heck, I can't even measure that low.. Quote:
When cable z exceeds load z, the inductive energy storage dominates...when load z is higher, capacitive storage dominates. While I do recommend matching load z, I understand the problem of speaker loads.. That's why it's best to compromise, get cable z in the middle of the range, while keeping (L*C)/1034 as close to 1 as is possible (L in nH per foot, C in pf per foot.). Foam based coax or foam dielectric spaced high aspect ribbons would be my choice. Quote:
But for those sitting in the sweetspot of a high end system, trying to discern soundstage imaging, I cannot share your blanket "enthusiasm". [QUOTE]Originally posted by Johan Potgieter [B]So, I would risk saying if an amplifier is prone to that kind of instability - redesign! Perhaps bold words, but I am an amplifier designer and cannot agree that such a state of affairs should necessarily exist. As a designer, you may choose to tradeoff stability for large signal bandwidth. That's a design call. Some designers believe bats should be happy as well, and are willing to give up some stability. Quote:
Not a bad thing, really. Just not my cup of tea. Cheers, John |
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