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Dave_M![]() HeadWizer Joined: Jul. 1, 2006 | Message [#100] posted on: 11-16-2006 01:44 PM CST (US). haha Cavalli Kan III worked out well It gets the thumbs up from me.But before you make the boards for this amp, you need to design 2 brand new amps, CKI and CKII first [Edited by Dave_M on 11-16-2006 at 01:48 PM.] |
runeight![]() ![]() ![]() Headphone Council Joined: Mar. 8, 2002 | Message [#101] posted on: 11-16-2006 01:48 PM CST (US). Dave_M, I was editing my previous post to answer about the Zi when you posted your most recent. See above. |
amb![]() ![]() ![]() Headphone Council Joined: Apr. 1, 2004 | Message [#102] posted on: 11-16-2006 04:01 PM CST (US).
I am considering this possibility if this is what people want. Since my β22 amp could also use these JFETs at the input it makes sense for me do so.
The rail capacitance before the regulator is so much higher than after, there is no chance that the regulators might see reverse voltage (unless if someone short circuits something, but then all bets are off). Since the PSU is integrated on the board, we don't have to worry about the scenario like with tangent's STEPS where someone might use the PSU to power something with a lot of additional capacitance. So, adding protection diodes in this amp would just be adding useless cost (albeit not a lot in terms of dollars, but they do use up PCB space).
The triangular pin configuration allows some flexibility if someone were to use transistors that don't have CBE or EBC pinouts. For example, many Japanese transistors have ECB pinout which could be mounted by turning the body, but a straight-tape configuration would not allow that without crossing the leads.
CRC or CLC are useful in unregulated supplies, but in a regulated supply I feel they are superfluous. Inserting resistance in series with the regulator increases voltage fluctuations according to current draw. Even though the second capacitor would absorb some of that, why introduce the fluctuations in the first place? |
amb![]() ![]() ![]() Headphone Council Joined: Apr. 1, 2004 | Message [#103] posted on: 11-16-2006 04:05 PM CST (US).
To give proper credit to the original designer I think we should keep the Kumisa name. Runeight and I are responsible for the mods, of course. Call it Kumisa Kan if you like, sort of like what Netscape use to say about its web browser "It's spelled Netscape, but it's pronounced Mozilla". ![]() [Edited by amb on 11-16-2006 at 04:06 PM.] |
runeight![]() ![]() ![]() Headphone Council Joined: Mar. 8, 2002 | Message [#104] posted on: 11-16-2006 07:04 PM CST (US). There was a question earlier about distortion. Here are some sim results. The usual caveats that sims are all perfect and that all devices of the same type are identical, the PS is perfect, etc, etc. For 40mW continous power into 32R at 1KHz (50mA peak current) I get: 2kHz - .015% Zo ~= 0R4 These results are for 60mA idle current in the output transistors. These are pretty good sim results for an amp with no feedback. I see that amb is already leaving me out of the name (clever as it is). [Edited by runeight on 11-17-2006 at 12:24 AM.] |
amb![]() ![]() ![]() Headphone Council Joined: Apr. 1, 2004 | Message [#105] posted on: 11-16-2006 07:12 PM CST (US).
LOL, that was strictly unintentional of course. |
Dave_M![]() HeadWizer Joined: Jul. 1, 2006 | Message [#106] posted on: 11-17-2006 11:10 AM CST (US). Are those sim results for BJT or JFET input? Or doesn't it matter? Also, going back to input impedance for BJT version.. if you consider the input impedance of just the amp and don't include the pot, because from the amp's point of view, the pot is part of the source (I think that is the case). And say you had a 100k pot, then it would be possible for the output impedance of the source (including pot) to be higher than the input impedance of the amp? What I'm trying to say is, for the BJT version, it is better to use a low value pot like 10k? because in audio you usually want the output impedance to be lower than the input impedance of the next stage. |
runeight![]() ![]() ![]() Headphone Council Joined: Mar. 8, 2002 | Message [#107] posted on: 11-17-2006 02:46 PM CST (US). The distortion results are with the jfet input. The introduction of the vol pot is actually a little more complicated than we've discussed and what it does depends on which point of view you take, the source or the sink (amp). Most vol pots are drawn vertically with the wiper shown somewhere along the resistor. Let me call the part above the wiper connected to the source the "top" and the part below the wiper connected to ground the "bottom." What we really have is the source's output inpedance in series with the top part of the vol pot. These two series resistors are then in series with a third resistor made from the bottom part of the vol pot in parallel with the input impedance of the sink (the amp). As in this diagram:
From the amp's point of view it has a Zi of the paralleled resistor. It then sees a source whose Zo is the sum of the actual Zo plus the top part of the vol pot. From the source's point of view it sees a load resistor consisting of the top part of the vol pot in series with the paralleled resistor made from the bottom part in parallel with the actual Zi of the amp. Thus, what each part (source or amp) sees depends on where the vol pot is set. This also means that the freq response of the front end of the amp can depend on where the vol pot is set since the top portion of the vol pot is in series with the capacitances of the front end. This may be noticeable if there is a large Miller capacitance, but most of the time is not. All this to say that, yes, when the vol pot is set low, from the amp's point of view, there can be a much larger source impedance than the effective input impedance of the amp. But, what really matters is what does the source see?? Because it's the loading effects on the source that we are generally concerned with. And the source sees at best the full resistance of the pot (volume set to zero) to at worst the parallel resistance of the pot and Zi (volume set to max). If the Zi of the amp is 100k and the pot is 100k then the source sees at best 100k (min volume) and at worst 50k (max volume). MHO is that it is generally better for the vol pot to be bigger to increase the value of the load that the source sees. But this must be balanced against the series resistance that the pot puts at the input and the attendant increase in noise and the affect on freq response. Otherwise we would just make the pots 10M to have a very high input impedance to the amp. So for this reason and others that probably go back to early tube designs, we tend to stick with 50-100k for the volume controls. [Edited by runeight on 11-17-2006 at 05:26 PM.] Attachment: C2307.gif |
Dave_M![]() HeadWizer Joined: Jul. 1, 2006 | Message [#108] posted on: 11-17-2006 08:21 PM CST (US). Thanks for that detailed reply. I assumed that loading the source a bit more was not a problem and 10K load was still high enough. One solution would be to use a pre-amp between the pot and the amp input Or a much better solution would be to have JFET input on the amp. oh wait.. you thought of that already ![]() |
| disfunctionalshadow Member Joined: Nov. 20, 2006 | Message [#109] posted on: 11-20-2006 08:46 PM CST (US). I'm curious as to why 3.3K is used for the CFB output stage (R20/R22)? The few times I worked with that topology on power amps those Thanks |
dBel84![]() ![]() HeadWize Fanatic Joined: May 5, 2006 | Message [#110] posted on: 11-20-2006 09:57 PM CST (US). My understanding is based on the link listed below. The value of the resistor sets the current and load in the first transistor and it is a good compromise for linearity versus distortion ... http://www.dself...iscrete/cfp.htm I am sure Runeight and others can shed more light..dB |
| disfunctionalshadow Member Joined: Nov. 20, 2006 | Message [#111] posted on: 11-21-2006 12:14 AM CST (US). Thanks dB. I hadn't seen that page, though I've read Doug's book and the graphs he shows in there were only for 50 ohms to 100 ohms. Of course that's power amps with a higher standing bias and driving much heavier loads. But I first saw CFB in the Amber Series 70 amps that used |
amb![]() ![]() ![]() Headphone Council Joined: Apr. 1, 2004 | Message [#112] posted on: 11-23-2006 05:54 AM CST (US). An alternative to the Amveco transformer listed in the BOM, is the Avel-Lindberg Y236003 (15V+15V 15VA). This is rated double the required capacity, but is still compact enough to fit in the Hammond 1455Q220x case along with the amp PCB. FYI. |
amb![]() ![]() ![]() Headphone Council Joined: Apr. 1, 2004 | Message [#113] posted on: 11-24-2006 07:33 AM CST (US). An update: I am beginning to do spice simulations of the CKIII amp and will post results very soon. After runeight and I are both happy with everything, I will get ready to order boards. Stay tuned. |
amb![]() ![]() ![]() Headphone Council Joined: Apr. 1, 2004 | Message [#114] posted on: 11-24-2006 07:04 PM CST (US). Here are some simulation results. The amp's output stage is biased to flow 30mA at idle, and the output is loaded with 32Ω. In order to achieve 30mA quiescent current, I had to reduce the Vbe multiplier resistor R18's value slightly. To provide a wider adjustment range, I conferred with runeight and we have decided to change R18's value to 2.4KΩ and the R19 trimpot to 1KΩ. Runeight will post an updated schematic reflecting this change. The following is the frequency response and phase response graph. The response is flat within the audio band. In the subsonic region, a peak is observed, reaching a maximum of 1.3dB at 1.17Hz, below which the response falls sharply. This is due to DC servo action. At the ultrasonic end, the -3dB point is 1.96MHz. Since the input is 1V, the graph shows that the gain of the amp is almost exactly 9x (19dB). The phase response is also flat within the audio band, +20° at 1Hz, -4.4° at 100KHz, and -43° at 1MHz.
Here is a harmonic distortion spectrum, with a 1KHz fundamental, and the input level adjusted to produce 1Vrms (1.4142V peak) at the output. Only the 2nd and 3rd harmonics are significant, at 0.0085% and 0.013%, respectively. None of the higher order harmonics exceed 0.0013%.
Below is the output impedance vs. frequency plot. The Y-axis is labeled as millivolts but is actually in milliohms. The output impedance is about 0.46Ω over the entire audio band, with a peak and rolloff in the subsonics due to the DC servo.
The 100KHz square wave response is shown below. It is characterized by fast slewing and gentle settling with no overshoot and ringing.
Attachment: C2329.png,C2330.png,C2331.png,C2332.png |
runeight![]() ![]() ![]() Headphone Council Joined: Mar. 8, 2002 | Message [#115] posted on: 11-24-2006 10:54 PM CST (US). And here are the updated schematics. I guess that amb is about ready to offer boards. Between this amp and the b22 he has a lot to do. ![]() This amp performs exceedingly well for a no NFB amplifier. I think that you guys are going to like it. Attachment: C2334.gif,C2335.gif |
Clutz![]() ![]() HeadWize Fanatic Joined: Jun. 1, 2002 | Message [#116] posted on: 11-25-2006 11:12 AM CST (US). I know amb has said before that there isn't anything wrong with feedback; but for the moment, what are the arguments against using feedback, just out of curiousity? |
runeight![]() ![]() ![]() Headphone Council Joined: Mar. 8, 2002 | Message [#117] posted on: 11-25-2006 05:02 PM CST (US). There really isn't anything wrong with feedback. It's just a tool in circuit design that can be used under the right circumstances to get better performance from a particular amp topology. However, there are those who hate NFB in all its guises and those who don't mind using lots of it (as in the b22 and SS power amps) and those who use some amount of it (as in many tube power amps). There are many, many opinions on the sound of NFB. The main features of global NFB are that it theoretically 1) reduces harmonic distortion, 2) lowers the output impedance and 3) increases the bandwith. These are all good things, but like many other things in the world of audio, you can't make bad amp into a good one by simply applying NFB. You can't make a bad amp into a good one by using boutique components. Over the years, lots of designs, particularly SS amps, have simply used massive amounts of NFB to cover up a bad design and/or crappy components. Consequently NFB is often associated with really bad sounding SS amplifiers. OTOH, a well designed amp, such as the b22, can be made better with NFB. How much NFB depends on the particulars of the design. Even though NFB does those three great things listed above, it is not without its own inherent problems. There are three of these that I know about. One is that after a while all amps with lots of NFB tend to sound the same. At least I have heard this from others who have listened to a wide variety of amps. And this is believable to me. The second problem is that when you send the output of an amp back into its input you don't get perfect NFB because there is a phase lag as the signal traverses the amp to the output and back into the input. Because of the phase lag you don't get perfect NFB type cancellation of non-linearities introduced by the amplifier. Instead, because of the phase differences, you can get even worse intermodulation components that diminish or destroy the good effect of the NFB. The third problem is that there is always a phase shift in the ultrasonic realm where, eventually, the phase shift goes to 180d. At this point the amp will oscillate and so the NFB loop has to be compensated to hammer this oscilation, generally with a cap in parallel with the feedback resistor and, in tube amps, a forced rolling off of the gain of the input stage below the critical frequency. I called this a problem. It is not really a problem, but just a design detail that has to be handled. So, you can't make a bad amp better by just slinging NFB into the circuit. But you can apply NFB to a properly designed amp to get better results. If you look at amb's b22 graphs, you'll see that the amp has almost no phase shift in the audio band and that it is very fast. This means that you can apply a fair amount of NFB without suffering from the bad effects of NFB. There is about 40db of NFB in the b22 and the actual performance measurements indicate that the amp is doing better because of this. This is because amb first designed a very good, low distortion, high speed, medium gain amplifier before applying global NFB. Some would argue that even with this good behavior in the audio band, there is increasing phase shift in the ultrasonic region that will create intermodulation components. I don't know what effect this may or may not have. I guess this was a long answer to the question. The short answer is that NFB is neither good or bad, it's only the particular application of it makes it one or the other or somewhere in between. I am pretty sure of one thing. Almost every commercial power amp that you've ever heard has NFB and you have, therefore, heard what is "sounds" like. Of course, no one would ever use NFB if the active components in the amp did not generate inherent distortion because there would be no reason TO use it. Most, if not all of the opamp-based amplifiers that are popular use some amount of NFB. In general this happens even when a discrete buffer is used because the buffer is inserted into the global feedback loop of the opamp so that the opamp can zero the offset. We don't even think about using NFB with opamps because it's the only way to control their gain, but many would consider opamps to be poor audio amps because of this NFB. With regard to the CKIII and no NFB. It can be a real challenge to design a good amplifier with no NFB and low THD and low Zo. The CKIII has these qualities. Its THD is quite low and its Zo is not bad. Since we don't want to use NFB unless we MUST use it, the CKIII falls into a category of an excellent amp that does not use NFB. There are members of this forum who are far more knowledgable than I am about the details of NFB. Hopefully they will also take time to answer and correct any errors in my explanation. [Edited by runeight on 11-25-2006 at 05:12 PM.] |
amb![]() ![]() ![]() Headphone Council Joined: Apr. 1, 2004 | Message [#118] posted on: 11-25-2006 07:00 PM CST (US). Runeight has written a very good explanation. The only thing I would elaborate on, is the term "NFB" here refers to global negative feedback. The CKIII does not employ global negative feedback, but has local negative feedback (sometimes also known as "degeneration"). Without local negative feedback then the amp would have unpredictable gain characteristics (which is highly dependent on the transistors used), and most likely too much gain to be usable in our application. In the CKIII, the gain is partially determined by the ratio of R12/R11 (and R13/R14), because even though Q7 and Q8 are each half of a current mirror, they are also common-emitter amplifiers. Since there is no global loop, the gain of the amplifier is the "open loop" gain, and a comparatively large amount of local feedback must be used to set the gain appropriately. The benefit is that there is no propagation delay to worry about (and a host of associated issues that must be addressed), the drawback is that local feedback isn't as effective in suppressing distortion and lowering output impedance as global feedback. DC stability is another issue that is a problem in an amp with no global feedback, and the CKIII solves the problem with its DC servo. The CKIII otherwise performs exceedingly well for an amp with no global feedback. Both local and global negative feedback are utilized in the β22. Local feedback is used to control the gain of each individual stage of the amp (so that a moderate target open loop gain is achieved), while global feedback is applied to set the overall closed loop gain (and to achieve the performance enhancements that runeight has mentioned). This is quite different than the approach taken in some designs where the open loop gain is made as high as possible, so that a large amount of global feedback is applied (the amount of global feedback is the difference between the open and closed loop gains). Pretty much any opamp-based design will fall into the latter category, where the opamp's open loop gain could be as high as 120dB or more, forcing a large amount of global feedback. [Edited by amb on 11-25-2006 at 07:08 PM.] |
runeight![]() ![]() ![]() Headphone Council Joined: Mar. 8, 2002 | Message [#119] posted on: 11-25-2006 08:58 PM CST (US). Yes, what amb said. There is quite a lot of local NFB in the CKIII, in the current mirrors as amb noted and also in the CFP output pairs. The optional capacitors on the schematic attached to the CFP pairs are for dealing with the high-freq instability that can occur from the very large amount of local NFB, although this doesn't appear to be a problem in this particular amp topology as it sometimes is in power amps.So now you guys have two new amazing amps to choose from. Each from a completely different design perspective. The b22 from the perspective of an extremely well done basic amp expressly designed to have substantial global NFB (with a new, fast PS to go with it). The CKIII from the perspective of an amp expressly designed to have no global NFB (with PS all on a single board). Or you can build both of them and compare. [Edited by runeight on 11-25-2006 at 11:12 PM.] |
Clutz![]() ![]() HeadWize Fanatic Joined: Jun. 1, 2002 | Message [#120] posted on: 11-26-2006 12:39 AM CST (US). You guys answered my questions perfectly, thank you. As with a lot of things in hifi audio, there seems to be a lof of dogmatic opinions on the "right' way of doing things, and I've often noticed that when you ask people on one side of the argument about the other - they give an incomplete, or distorted picture. I really appreciate the effort you guys put into this response. ![]() Bottom line is - now I want to build both |
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