You forget to mention you were going to type s l o w l y .Jaka Racman said:I will try to use simple analogies so you IT guys might understand.
Take it from 'us IT guys', you need to improve on your condescending tone: it's not quite sharp enough to be funny and insulting at the same time.
The issue can be summarized as energy in = energy out, so the class D amp will draw less power than the class AB for the same output.
Not quite. I'm not any wiser than I was today at 12:16 PM. I think richie00boy got the general idea as well, even if he got a few details wrong. Time to revise your ideas on these 'IT guys'? 😎Jaka Racman said:Mission accomplished.
richie00boy said:The way that class-d works is to draw the max current with every pulse, but the duration is such that it averages out to be the same average current that a class-b amp would draw. Class-d amps are more efficient in heat terms not electrical power drawn from the supply. Therefore the transformer for a class-d amp cannot be any smaller than that for a class-b amp.
Using your example, going down the sinewave say to halfway, the class-b amp will be drawing half the max current, but the class-d amp will draw the max current but only for half the time. Thus as far as the load upon the supply they are both the same. The fact that the class-b transistors will also have half the supply voltage across them means that they will get hot, whereas the class-d amp will have very little voltage across them, so it runs cool.
More efficient in heat terms means that they need less power!!!
Gertjan
Originally posted by Hans L
I think richie00boy got the general idea as well, even if he got a few details wrong.
Originally posted by richie00boy
The way that class-d works is to draw the max current with every pulse, but the duration is such that it averages out to be the same average current that a class-b amp would draw.
The above quote shows total lack of comprehension how classD amplifier actually works. Now if you would substitute current for voltage, that would be correct. Namely:
The way that class-d works is to supply the max voltage with every pulse, but the duration is such that it averages out to be the same average voltage that a class-b amp would produce.
Amplitude of current pulses is actually the same as coresponding load current at the same time, or the same as class B amp would produce. (inductor ripple current is neglected in this explanation.) So we have a series of current pulses whose envelope coresponds to that of a class B amp curent consumption, but whose average value is less than envelope. This is where the conversion process of classD amplifier takes place and that is why it can be compared to a variable transformer. Actually duty cycle corresponds to turns ratio of such a variable transformer.
Now if you still think those are minor differences, then there is also a minor difference between classD and classA (both being amplifiers) and we can end this discussion.
Best regards,
Jaka Racman
Attached is image of current pulses drawn fom power supply in classD amp.
Attachments
Thanks Hans.
Thank you Jaka for the explanation. I may have mangled my words a little, but from your post it seems that my thinking was along the right lines. The point being that the amp, whether it is class-d or class-b, draws the same amount of current from the supply in the grand scheme of things. So if the toroid voltage is the same for a class-d or class-b amp (which it will be for all intents and purposes) then the VA requirement of the toroid must also be the same for a class-d or class-b amp. Is this assumption correct or have I messed up again?
Thank you Jaka for the explanation. I may have mangled my words a little, but from your post it seems that my thinking was along the right lines. The point being that the amp, whether it is class-d or class-b, draws the same amount of current from the supply in the grand scheme of things. So if the toroid voltage is the same for a class-d or class-b amp (which it will be for all intents and purposes) then the VA requirement of the toroid must also be the same for a class-d or class-b amp. Is this assumption correct or have I messed up again?
Hi richie00boy,
I am afraid that your assumption is incorrect. The point is that the current drawn from the power supply is average value of the waveform. I attach two waveforms, black one showing current drawn by classD amp and red one showing output (load) current of the same amp. Load current would be the same as current drawn by classB amp. In upper right corner you see calculated average values of both currents, 4.23A for classD and 6.26A for classB. (Average value is calculated as area of the waveform, so you must account for the voids between current pulses.) As you can see, there is 2A difference between both amps. Those 2A of current is transferred into heat in the classB amp, so this is why classD amp runs cooler: It draws less current from the power supply.
Best regards,
Jaka Racman
I am afraid that your assumption is incorrect. The point is that the current drawn from the power supply is average value of the waveform. I attach two waveforms, black one showing current drawn by classD amp and red one showing output (load) current of the same amp. Load current would be the same as current drawn by classB amp. In upper right corner you see calculated average values of both currents, 4.23A for classD and 6.26A for classB. (Average value is calculated as area of the waveform, so you must account for the voids between current pulses.) As you can see, there is 2A difference between both amps. Those 2A of current is transferred into heat in the classB amp, so this is why classD amp runs cooler: It draws less current from the power supply.
Best regards,
Jaka Racman
Attachments
It's really very simple: less losses in the class D amp mean less power consumption for the same power output.
Sorry guys for the lengthy detour. Back to the topic: UcD180
I order 6 of them, 2 of them with the opamp upgrade and they arrived a few days ago 🙂. I've been reading most of what has been posted on the 180/400/ucd in general. There's a lot and it's all cut up in pieces with sound and maybe not so sound advice, which is for the reader to decide. I've clinged onto Bruno's posts for reference. Who would know better than the designer, right? It had one good effect: it made me pick up a few books on electronics to get a better understanding myself. I don't like fishing in the dark.
Question1:
I've already read one comparative review on the 8620 upgrade. Have there been more subjective listening test in the meanwhile? I'm presuming the biggest advantage it will have in in the mid or maybe only in the high frequencies. Am I right?
Question2:
The easy to implement softstart circuit presented -here-, does it have any sonic disdavantages against for instance the more elaborate module found at lcaudio. In other words, once the relais has been closed, could the circuit still have an effect on the power supply?
Thanks.
I order 6 of them, 2 of them with the opamp upgrade and they arrived a few days ago 🙂. I've been reading most of what has been posted on the 180/400/ucd in general. There's a lot and it's all cut up in pieces with sound and maybe not so sound advice, which is for the reader to decide. I've clinged onto Bruno's posts for reference. Who would know better than the designer, right? It had one good effect: it made me pick up a few books on electronics to get a better understanding myself. I don't like fishing in the dark.
Question1:
I've already read one comparative review on the 8620 upgrade. Have there been more subjective listening test in the meanwhile? I'm presuming the biggest advantage it will have in in the mid or maybe only in the high frequencies. Am I right?
Question2:
The easy to implement softstart circuit presented -here-, does it have any sonic disdavantages against for instance the more elaborate module found at lcaudio. In other words, once the relais has been closed, could the circuit still have an effect on the power supply?
Thanks.
- except that at low power output, the efficiency rivals the low bias Class AB because of the considerable heat loss through the output filter, something almost never mentioned about Class D.
Cheers,
Hugh
Cheers,
Hugh
I see a jaw-dropping Hans in his home theatre in the future?
Not many will be able to compare the improved modules vs the standard ones - but you can!
Listening tests are hard to do, if you have a positive mind about the modules and you disconnect your old amp, there's already the placebo effect.
I always thought well-built amps are all very close together, as long as they are not underpowered or rightout badly designed, they sound the same. I've learnt otherwise by reading just how many class AB designs are possible (feedback, bias level, current limiting, etc)
I can't say much yet, I've only done very limited single channel tests with b&w speakers and my old Philips speakers, the other speakers I tested don't have the resolution to show anything.
Both these speakers are larg(ish) floorstanders - The Philips I couldn't compare because I haven't heard them on my old system since october. The Philips did sound very tight in the bass, but it could be placebo effect or just the track being played (and they weren't in the same spot I'm used to hearing them)
The B&W Nautilus was in the same spot. It had a lot of authority playing a St. Germain track. The change was not subtle, it was even more revealing to switch back to my old amp. The difference is best described as "less tight"
I'm looking at the same soft start you are - the sound doesn't seem to be a concern, as long as the relay can handle the amps it should be fine - however, I wonder how long it takes for the caps before the relay will drain - if power cycles fast (like 5 seconds or so between off and on) the relay might still be engaged... maybe a resistor parallel over the relay?
About DC protection, i'm still thinking about the vellemans, they should do the job nicely, but it's a lot of stuff parallel on the speaker path, I'm afraid it will have sound - haven't seen any opinions on those in here - except on another forum, they are reported to "s*ck"

Not many will be able to compare the improved modules vs the standard ones - but you can!
Listening tests are hard to do, if you have a positive mind about the modules and you disconnect your old amp, there's already the placebo effect.
I always thought well-built amps are all very close together, as long as they are not underpowered or rightout badly designed, they sound the same. I've learnt otherwise by reading just how many class AB designs are possible (feedback, bias level, current limiting, etc)
I can't say much yet, I've only done very limited single channel tests with b&w speakers and my old Philips speakers, the other speakers I tested don't have the resolution to show anything.
Both these speakers are larg(ish) floorstanders - The Philips I couldn't compare because I haven't heard them on my old system since october. The Philips did sound very tight in the bass, but it could be placebo effect or just the track being played (and they weren't in the same spot I'm used to hearing them)
The B&W Nautilus was in the same spot. It had a lot of authority playing a St. Germain track. The change was not subtle, it was even more revealing to switch back to my old amp. The difference is best described as "less tight"
I'm looking at the same soft start you are - the sound doesn't seem to be a concern, as long as the relay can handle the amps it should be fine - however, I wonder how long it takes for the caps before the relay will drain - if power cycles fast (like 5 seconds or so between off and on) the relay might still be engaged... maybe a resistor parallel over the relay?
About DC protection, i'm still thinking about the vellemans, they should do the job nicely, but it's a lot of stuff parallel on the speaker path, I'm afraid it will have sound - haven't seen any opinions on those in here - except on another forum, they are reported to "s*ck"

Jaka Racman said:Hi richie00boy,
I am afraid that your assumption is incorrect. The point is that the current drawn from the power supply is average value of the waveform. I attach two waveforms, black one showing current drawn by classD amp and red one showing output (load) current of the same amp. Load current would be the same as current drawn by classB amp. In upper right corner you see calculated average values of both currents, 4.23A for classD and 6.26A for classB. (Average value is calculated as area of the waveform, so you must account for the voids between current pulses.) As you can see, there is 2A difference between both amps. Those 2A of current is transferred into heat in the classB amp, so this is why classD amp runs cooler: It draws less current from the power supply.
Best regards,
Jaka Racman
Jaka,
Thank you for that explanation, it was exactly what I was looking for. I guess the average current for the class-d amp will depend on the topology, or will all class-d amps have an average current that is x amount of the class-b average current?
Originally posted by richie00boy
I guess the average current for the class-d amp will depend on the topology, or will all class-d amps have an average current that is x amount of the class-b average current?
Hi richie00boy,
the answer is not very simple. In theory, Class D amplifier is a power conversion device and can theoretically be 100% efficient, that means that all the power from the source is transferred to the load without being wasted in the amplifier. That would be invariant of the topology of classD circuit.
In practice, for almost all comercially available classD amps only so called step-down (buck) topology is used. And because real devices are used as switches, there are also losses in those devices, which are subdivided into conduction and switching losses. So for comparing various classD implementations a factor of merit is used called efficiency
efficiency = power delivered to the load / power drawn from power supply
or
efficiency = power delivered to the load / (power dissipated in the amp + power delivered to the load)
For good classD amps, efficency is somewhere between 0.92 to 0.96 at full power, maybe even better for subwoofer amps. Sadly efficiency is not constant over the whole output power range (as Hugh has kindly noted) and is lower at low output powers because some losses are fixed and independant of output power level. On the good side, efficiency of classD is independant of the load phase angle.
Efficiency can equally well be applied to classB amplifiers. Here efficiency is is even more trickier to define over whole power range, since it depends on output power, shape of output waveform and load phase angle. In general, efficiency improves with output amplitude and reaches maximum of .78 (IIRC) for sinusoidal signal at full output power. It can be even grater with square wave signals.
Now your question was about dimensioning of power supply transformer. For continious output power, you dimension your transformer for load power + power dissipated in amp. Now this can simply be calculated as:
power required = maximum load power / efficiency
So for typical classD you need 1.06 times load power and for classB 1.28 times load power. As you can see, the difference is not that great, but it still exists.
Best regards,
Jaka Racman
Originally posted by Jaka Racman
In theory, Class D amplifier is a power conversion device and can theoretically be 100% efficient, that means that all the power from the source is transferred to the load without being wasted in the amplifier. That would be invariant of the topology of class D circuit.
For good class D amps, efficiency is somewhere between 0.92 to 0.96 at full power, maybe even better for subwoofer amps. Sadly efficiency is not constant over the whole output power range (as Hugh has kindly noted) and is lower at low output powers because some losses are fixed and independent of output power level. On the good side, efficiency of class D is independent of the load phase angle.
Efficiency can equally well be applied to class B amplifiers. Here efficiency is is even more trickier to define over whole power range, since it depends on output power, shape of output waveform and load phase angle. In general, efficiency improves with output amplitude and reaches maximum of .78 (IIRC) for sinusoidal signal at full output power. It can be even grater with square wave signals.
So for typical class D you need 1.06 times load power and for class B 1.28 times load power. As you can see, the difference is not that great, but it still exists.
Hi Jaka,
A few points: 1) I admire your knowledge and gentle patience; 2) in the ear of my mind your name has a soft "J" (like the German "Ja") and a hard "c" (like a "k") - am I "hearing" that correctly?; 3) perhaps your diplomatic nature is leading you to understate the efficiency difference between the B and D classes of amplifiers. Your estimation of the efficiency of a typical class D design seems correct, but, in my experience, a typical class B amp will be lucky to achieve fifty percent (near forty is more likely) when operating with best case real music (highly compressed techno) into a real load (at least thirty degrees inductive) at maximum listenable output (ten percent clipping). So the size ratio of the transformers will be closer to 2:1. And the ratio for heat sinks will more like 10:1.
Regards, analogspiceman (note: the "spice" is sharp)
Hi anlogspiceman,
Your pronunciation is correct and I agree with everything you have writen. I forgot to mention that my figures would be correct if the transformer would be dimensioned in an industrial way (for continious operation with maximum output power and sinusoidal signal). Class B has worst efficiency at half output power (only 0.5), and given dynamic nature of music signal it will most likely operate around this point when pushed to the limit. For anyone interested, here is link to the Rod Elliot's page discussing classB efficiency.
On the other hand classD should maintain high efficiency over much broader range (over 0.9 above 20 or 30% of output power) so it's heatsink (and transformer) can be considerably smaller.
Since Bruno gave some insight how transformers in audio are dimensioned nowadays (FTC testing at only 1/8th of rated output power), your figure would seem correct for transformers that are dimensioned for music signals.
Best regards,
Jaka Racman
Your pronunciation is correct and I agree with everything you have writen. I forgot to mention that my figures would be correct if the transformer would be dimensioned in an industrial way (for continious operation with maximum output power and sinusoidal signal). Class B has worst efficiency at half output power (only 0.5), and given dynamic nature of music signal it will most likely operate around this point when pushed to the limit. For anyone interested, here is link to the Rod Elliot's page discussing classB efficiency.
On the other hand classD should maintain high efficiency over much broader range (over 0.9 above 20 or 30% of output power) so it's heatsink (and transformer) can be considerably smaller.
Since Bruno gave some insight how transformers in audio are dimensioned nowadays (FTC testing at only 1/8th of rated output power), your figure would seem correct for transformers that are dimensioned for music signals.
Best regards,
Jaka Racman
While I'm not getting any answers to my questions and you are having a blast with differenct classes of amps, I might as well go back to meta communication...
Since when is taking a cheap stab at one person and opening the next post with an insult towards two ppl considered gentle patience and of diplomatic nature??? There are some funny social rules going on here. Since analogies are in, try this one: 'If you are One-eye in the land of the blind, you get to smack anyone you meet and still be praised for you peaceloving nature.'
Since when is taking a cheap stab at one person and opening the next post with an insult towards two ppl considered gentle patience and of diplomatic nature??? There are some funny social rules going on here. Since analogies are in, try this one: 'If you are One-eye in the land of the blind, you get to smack anyone you meet and still be praised for you peaceloving nature.'
Hans,
I've posted a listening test on Ucd400AD's in the UcD400 thread. Of course, keep in mind it's highly subjective and compared to 2*90W/8 ohm channels of a receiver. The dynamics I experienced could be due to the double power UcD400 provides (quite a few db's headroom extra)
Yves
I've posted a listening test on Ucd400AD's in the UcD400 thread. Of course, keep in mind it's highly subjective and compared to 2*90W/8 ohm channels of a receiver. The dynamics I experienced could be due to the double power UcD400 provides (quite a few db's headroom extra)
Yves
Hi Hans,
Question one, Since you cling to what Bruno say's, you'll notice he's spoken of that op amp rather highly, may as well go with that opinion.
Question 2: How is that different from the LCaudio one? I've never seen an actual schematic of it.
That simple one though, leaves nothing in the path of the signal other than the relay contacts, even if there were any noise induced by that (doubtfull I think), it still goes through your power supply and all the amps local bypassing, so I think it's safe to say it would have zero audible effects.
Regards,
Chris
Question one, Since you cling to what Bruno say's, you'll notice he's spoken of that op amp rather highly, may as well go with that opinion.
Question 2: How is that different from the LCaudio one? I've never seen an actual schematic of it.
That simple one though, leaves nothing in the path of the signal other than the relay contacts, even if there were any noise induced by that (doubtfull I think), it still goes through your power supply and all the amps local bypassing, so I think it's safe to say it would have zero audible effects.
Regards,
Chris
Thank you Yves (and for your previous reply). I will look up your review of the UcD400AD. The 400 is supposed to sound pretty much the same as the 180 so I'm sure the difference you describe should be what I may expect.
Classd4sure, I don't have a schematic of the LCaudio module either. Was hoping someone could shedsome light on it, but I think it's safe to say they are rather expensive and might not be fundamentally different at all.
I don't have enough understanding of electronics to judge what a 'loose hanging' capacitor or other parts, once the relais is closed, may invoke on a circuit. Thanks for clearing that up. It seems to be a superb diy choice, it's simple and cheap and does exactly what one needs. I guess the only thing worth spending a few bucks more on would be the relais (solid contact over the years). One thing I would think of doing is use multiple resistors in parallel (instead of the series resistors) across the relais for better power handling and aim for a higher total resistance just to be on the safe side.
Classd4sure, I don't have a schematic of the LCaudio module either. Was hoping someone could shedsome light on it, but I think it's safe to say they are rather expensive and might not be fundamentally different at all.
I don't have enough understanding of electronics to judge what a 'loose hanging' capacitor or other parts, once the relais is closed, may invoke on a circuit. Thanks for clearing that up. It seems to be a superb diy choice, it's simple and cheap and does exactly what one needs. I guess the only thing worth spending a few bucks more on would be the relais (solid contact over the years). One thing I would think of doing is use multiple resistors in parallel (instead of the series resistors) across the relais for better power handling and aim for a higher total resistance just to be on the safe side.
IMO a soft start using a relay will not have any influence on the sound as it's far too removed from the audio, firstly by a transformer then by a bank of smoothing caps. Be wary of using parallel resistors instead of series as they will need to be rated for the full mains voltage which will not be easy to find; that's why people use series.
Series will still have the same power handling. Also beware of increasing the resistance, if you increase it too much the PSU caps will barely have charged during the soft start period so when the relay closes you get another surge.
If you fancy making your own board I have designed one that uses a very simple circuit, which I am just finalising. You are welcome to the layout if you want it.
Series will still have the same power handling. Also beware of increasing the resistance, if you increase it too much the PSU caps will barely have charged during the soft start period so when the relay closes you get another surge.
If you fancy making your own board I have designed one that uses a very simple circuit, which I am just finalising. You are welcome to the layout if you want it.
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