New Amplifier - ULD Extreme

Status
This old topic is closed. If you want to reopen this topic, contact a moderator using the "Report Post" button.
Member
Joined 2002
Paid Member
Re: ULD Extreme

sandyK said:
Greg
If it ran that hot, I wouldn't be game to have it in the cabinet.
I do however leave the cabinet's perspex doors ajar a bit during hot weather. This small "oven" has the preamp sitting on top of it, so that I already have most of the benefits suggested by Dave.
Alex

Alex,

Have you ever mesured the temperature?

My heatsink is around 30C (class AB) and that feels only slightly warm. I would have thought another 20C (class A) would be in the ball park.

regards
 
AKSA said:
Sebastien,

You are 100% correct. Those diodes should be back to back, and across the 220uF shunt fb cap.

Dave,

As frequency rises, the input impedance to the base of the VAS drops, and the local feedback via the Miller cap reduces gain. These conspire to increase distortion, no?

Cheers,

Hugh



Hugh,

Exactly. But you have brought to my attention my unintended ambiguity. If loading increases does impedance go up or down?
Anyway I obviously meant to say that impedance drops by the magnitude of XC // Zin (VAS).


Cheers,
Dave
 
Greg Erskine said:


Dave, interested. I've been thinking the same thing but wouldn't it be equally as good for the input transistors. I think I read years ago that JC does something to stop the flow of air around the transistors to keep the transistor temperature constant.

I was thinking the transitors should be buried in the main heatsink and internal air flow restricted. The main heatsink would need to be reduced in size the increase temp a little. Poor capacitors.

Alex's amp probably already runs at greater than 55C. :hot:

regards


G'day Greg,

Trust all's well.

I have some PTR's and I'm going to use a modded version of the Jaycar temp switch kit. I should be able to hold temp to within 1 degree C.

Keeping LTP's constant might be usefull in some designs but in this design the LTP temperature has really no effect on gm and the tail current is determined by the active current source which is already temperature compensated. In any case the LTP are usually sailing close to the wind with 50V rails and 3mA so extra heating is not recommended.
Also, I'm trying to be as green as possible (within reason). For a 100W amp my E ULD runs very cool. I'm trying to keep it Peter Garrett friendly.

Cheers,
Dave
 
I think you have misunderstood Self's advice.
I have edition 2 so all my references date back to that revision.

Fig 2.6 plots the distortion comparison between no output capacitor and 6800uF feeding an 8r0 load.
The F-3dB of this 6800uF 8ohm combination is ~2.9Hz. The graph shows that distortion rises through the whole audio bandwidth, when capacitor coupled.
But, very significantly shows an upward slope below 50Hz.
He then swaps the 6800uF to 100mF and compares the two before and after plots, Fig 2.7.
This has moved the F-3dB down by a factor ~15 to ~0.2Hz. The comparison is very illuminating.
He then shows the comparison using a 4700uF cap and the upward slope now starts at ~200Hz, fig2.8.

This all relates to output capacitor coupling, but I feel that this is the introduction to the chapter on the effects of the NFB cap (distortion 8).

Fig 6.14 shows the distortion rising from ~140Hz and this corresponds to the graph, fig6.15, showing the LF roll off associated with the NFB cap and it's -0.7dB @ 10Hz.
He goes on to say
"Capacitor distortion in power amplifiers is most likely to occur in the feedback network blocking capacitor (assuming DC-coupled amplifier). .....The feedback capacitor therefore tends to be relatively large, and if not large enough the THD plot of the amplifier will show the characteristic kick up at the LF end."
This implies that using a large enough capacitor eliminates the feedback capacitor distortion.
Further on he says
"It is common for amplifiers to show a rise in distortion at the LF end, but there is no reason why this should ever occur."

He confirms how to achieve this elimination of feedback capacitor distortion (in AC coupled amplifiers)
"The value of C2 (the feedback cap in fig6.16) (220uF) gives a roll off with R9 (680r) that is -3dB at 1.4Hz. The aim is not an unreasonably extended sub-bass response, but to prevent an LF rise in distortion due to capacitor non-linearity..... 100uF degraded the THD @ 10Hz.......Band-limiting should be done earlier, with non-electrolytic capacitors"
He implies that the degraded distortion evident at 10Hz is not good enough and the suggested value for C2 is 220uF to eliminate distortion8.
At no time has he mentioned that the protective diode/s play any part in eliminating this LF distortion.
The whole mechanism depends on filtering the input to prevent any AC voltage across the NFB capacitor. No AC voltage is equivalent to no capacitor distortion. It's all achieved by sizing the DC blocking capacitors appropriately.
The input filter of fig6.16 is set to Rc=0.1s the NFB filter is set to RC=0.15s i.e. NFBrc >= sqrt(2)*INPUTrc.

The diode/s are there to limit the fault voltages that could damage the capacitor and/or the input stage. They are not placed there to reduce distortion.
 
AKSA said:
I cannot see that the EF between LTP and VAS is necessary. I would prefer to see it AFTER the VAS.
Self actually offers this alternative as equally good. Or he may indicate it performs better but at extra cost.
I think he chose EF before the VAS to reduce the cost of the overall amplifier.
Self also said that if the VAS is cascoded, that the EF must follow the VAS.
 
Andrew,

I use Black Gate NX caps in this position, with very low VW rating. I put back to back diodes across them simply to protect them in the event of an output device failure, where the fb node would otherwise swing to the rail voltage/gain.

Since this cap has very low ESR, the AC voltage across it is also very low, in fact any AC voltage across it is in fact distortion artefacts, as you point out. Thus Self's argument that the cap should be large to avoid the characteristic THD rise at LF is on the money.

In most jfet designs, this cap may be eliminated. I'm not aware of any documented evidence that the absence of an electro in this position improves SQ, but I'm all ears....

Cheers,

Hugh
 
AKSA said:
David,

Forr is always correct. He is 1 smart guy....

Y'know, I cannot see that the EF between LTP and VAS is necessary. I would prefer to see it AFTER the VAS.

Thoughts?

Hugh

Hugh,

From a THD pov the EF seems to give the best bang for buck between LTP and VAS. There was some good info published by Self in EWW (and in his bible) which you may already have. By boosting the current gain the output impedance of the VAS is made small (xc / beta) By making beta > 20000 it's possible to reduce VAS output impedance to < 50 ohms at 2 KHz. You have probably achieved similar with your CFP VAS too but whether it accounts for the same level of SQ improvment as I've heard with blameless designs I don't know. But it definitely can't hurt.

Self found that buffering the VAS also reduced distortion but not quite to the same extent. Also, the more EF stages you have following the VAS the more you need to stabilise - assuming you use conventional bias gen from the VAS itself.
Another bonus with the EF beta booster is that the LTP is probably loaded with less miller capacitance because the device need only be small signal TO-92.
You are very correct to recommend substituting the bc 639 in the E-ULD200. That's really a poor choice by the SC design team.

Well not really my thoughts alone but who am I to disagree with with Mr Self. He was also attempting to design the simplest and least expensive amplifier. I'm sure there are much better designs but they would probably be much more complex. On the other hand it's reassuring to know that Candy's $50,000 Halcro's also resemble Self's 3 stage model.

FWIW the latest Krells do not employ class A but instead use high bias class A driver stages (very low Z out) to fully isolate the VAS from the crossover region. Perhaps that's a direction we could take the E-ULD200 - in due course. The self contained diode biasing of the output stage would make it more simple to implement a high bias class A driver stage. I'm thinking triple darlington with nested FB and dedicated bias control.
 
Page 91 of edition2.
"the VAS buffer is most useful when LF distortion is already low, as it removes Distortion4.......Two equally effective ways of buffering are shown in figures 41.7e and 4.17f"
fig4.17c is the beta enhancer.
prior to this he says
"It is hard to say which technique is preferable....... the beta enhancing emitter follower circuit is slightly simpler..... Either method, properly applied, will linearise a VAS into invisibility"
 
V2.0c ULD shows a string of 4diodes and a variable resistor (100r) along with 6NJLs.

Could a fifth and sixth diode be brought into the string but appearing in parallel to the VR?

The one or two extra diodes can easily be shorted out with a link if the builder does not want to use them.
The 100r can be any value from 100r to 20k.

This would allow the tempco to be dialled in by reduce the effect of the fifth diode by bypassing it with the VR.

None of this would take up any extra PCB space. It would increase enormously the options open to the first few builders, who could then advise the later builders on which options seem to work best.

I am sorry if this seems a repeat of what I said before, but it's a no cost option that has been ignored.
 
VHF man said:

FWIW the latest Krells do not employ class A but instead use high bias class A driver stages (very low Z out) to fully isolate the VAS from the crossover region.

;)

This is far more important than many people could think!
It took me a lot of time to figure out that a highly biased driver stage could change the fingerprint of a classic push-pull classB OPS towards classA sound
 
Status
This old topic is closed. If you want to reopen this topic, contact a moderator using the "Report Post" button.