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#11 | |
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diyAudio Member
Join Date: Feb 2003
Location: Jakarta
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Quote:
The capacitance usually determine the bass roll-off. Theoritically, several mF (3300 or so) is enough for 20HZ, but by listening you usually get more with higher capacitance, and it seemed like minimal distortion in the bass frequencies like PM said. The bass is clean (deep) but it seemed something is missing or the signal is delayed. Paralleling with smaller cap does solve this problem. And guess what? I'm more convinced of my strategy to parallel higher capacitor with... silver mica! (I put the micas right in the legs of the bigger caps) But it is the capacitor type or brand that matter more. In my previous post it is supposed to be Nippon-Chemicon, not Nichicon. |
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#12 |
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diyAudio Member
Join Date: Feb 2003
Location: Northern VA
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I have never used Silver Mica caps in signal path or for by-passing. Are they sonically better than film ones?
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#13 |
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diyAudio Member
Join Date: Jun 2002
Location: Left Coast
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Re Silver-mica, I don't think it is so much that they sound better as that they have different functional properties. First off the range of values is fro 1pF up to less than .1uF and generally you don't find many with a value greater than 1000-2000pF. At these smaller values, audio frequencies are blocked almost like DC so the chances you will ever use one in the audible part of the signal path is small. There isn't much overlap with film except for the smallest film values and largest silvmica values. The most likely alternative is Silver mica vs. ceramic. Their biggest advantage is tight standard tolerancwes and high stability compared to just about anything else.
They are pretty expensive so in the case of power bypassing, they are probably overkill. Also they are larger than ceramics. The only place I use them is as complensation capacitors. That's still not in the audible signal patrh but it is close enough that useing them there gives me reassurance. Most likely ceramics would work as well. I suppose that there *could* be some effect on what one hears in these applications if having very tight and stable values was important for a particular design. |
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#14 |
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diyAudio Member
Join Date: Feb 2003
Location: Jakarta
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sam9, how if the silmic effects is not analyzed from it's ability to work with audio frequencies, rather, from it's probability to affect electrolitic caps operation? And yes, I use small value silver micas.
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#15 |
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diyAudio Member
Join Date: Jun 2002
Location: Left Coast
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Jay,
I'm not sure I understand the the reference to electroliyics. If you mean why do you find the silver micas in parralel with electrolytics, I assume you mean when placed between the power rails and ground in parallel with an electrolytic. The principal reason is that the bandwidth of electrolytics is too low (perhaps 100kHz) to handle all the RF and other noise that might be catied by the power rails. A Silver Mica or ceramic in parallel extends the bandwidth to 100MHz or so. If electros were effective into the MHz spectrun, there would be no need for either Silver micas or cermic in this application. Silver micas or ceramics when used for compensation are used for a somewhat related reason, namely to control HF signals that get affect the feedback loop (both local and global). Without going into the details, the objective is to supress high frequencies starting somewhere around 50kHz and extending up into the MHz region. Although, you cannnot hear these, the transistors in an audio amplifier will react to them and runnaway oscillations can result. The audible significance to you is great -- these capacitors if choosen correctly keep the amp from literally going up in smoke! In most Amp designs the only capacitor that is *directly* in the signal path is the input decoupling capacitor. That's a completely different purpose entirely. If someone want's to explain this better or correct my errors, please do so. I'm responding within the limits of my understanding. |
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#16 |
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diyAudio Member
Join Date: Jun 2002
Location: Left Coast
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An after thought: look at www.avxcorp.com. Somewhere on this site is a table that describes some of the charateristics or various kinds of capacitors.
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#17 | |
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diyAudio Member
Join Date: Feb 2003
Location: Jakarta
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Quote:
Do you mean that the purpose of the input decoupling cap to block DC? Well, I have never cared enough to think about formulas or technical explanation behind these capacitors when I used them. That's because... it's just to complicated than doing a trial. Using silmic to bypass elyt caps in the signal path had never come across my mind until I read that silmic is the best at RF. So I thought why not give it a try in the decoupling of Opamp (low pass filter) from DAC high frequency output. Later I consistently use silmic to parallel elyt caps in the signal path. In certain output decoupliing situation I can hear clear difference when I paralleled the silmic with high capacitance elyts, not the "standard" MKP. For coupling (to ground) I still prefer paper or oil caps, and tantalum is just the worst. Well, there must be situations where tantalum is good (I used them once in RF), but in my audio experience, there are 2 types of caps that I found never been good enough for any applications: tantalum and the green small valued WIMA MKP. The latest are commonly used in audio gears ( )
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#18 |
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diyAudio Member
Join Date: Jun 2002
Location: Left Coast
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To begin with I've never seen a 1uF silver mica, even in a catalog. Every table, including the website referenced above says the max value for Silver Mica is >10nF (i.e, 0.01uF). You can try that in the audio output if you insist but I doubt you will care for the result, all a capacitor that small will pass is RF. If it is in parallel with another cap of 1uF or greater you will get most of the audio because the audio is passing through the larger cap.
BTW, 1uF will attenuate base somewhat - you really nead at least 4.7uF to avoid this. |
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#19 | |||
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diyAudio Member
Join Date: Feb 2003
Location: Jakarta
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Quote:
Quote:
And where did the 4.7uF come from? Was that in refference with Pavel's design? He himself reccommended a 10000uF instead of 4700uF as stated in the documentation, in parallel with 1uF~10uF. IMO, the capacitance theoritically should be: C = 1/(2.pi.F.R). With F=20Hz and R=8Ohm, I think it is close to 4700uF. But yes, I mostly use a 1/1000 of the bigger cap, so it is about 4.7uF when the bigger cap is 4700uF. I don't know how to come up with such number, it is just the "formula" I found in many designs. I didn't think that using less than 1uf or more than 10uF in parallel will create a problem in most situation (mainly as in the Pavel's amp). And because limited theories mostly cannot explain the phenomena around the use of the caps (and other areas of electronics too ), I have trusted my observations more than my knowledge. But if using 10pF in parallel with 4700uF will create a problem (e.g. in CDP output cap), I really want to know why.Quote:
I have a friend who is even worse. He not only tried different fuses in the transformer primary, even worse he tried different orientation of the fuse! I believe you will not try that. Me either.Cheers
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