• The move to the new server is done. There are some software and database maintenance updates in process. This has us passing the hat around to help out. We appreciate any donations. Seriously, even a dollar helps. The payment page may be found here - https://www.audiokarma.org/support.html

Does amplifier wpc @ 4 or 2 ohm really matter at "low" volumes?

At the very least, lodge your displeasure properly.

Anyways back to your problem. You have to think of an amplifier as a power reserve and a power delivery device in which signal and speaker are constantly drawing power and converting into cone movement. More cone movement calls for greater power draw. If the amp cannot keep up, fidelity degrades. So, you want an amp with good 2 and 4 Ohm ratings as a hedge against this. Will a high powered amp at 1 watt sound the same as at 50 watts? IME, yes. A low powered amp which typically has poor or non-existent 2 and 4 Ohm ratings will not be able to keep up and result in sag which can be heard as compression. You will not get the same sharpness or clarity.
I didn't see anyone disagreeing with that. But it is a discussion of low impedance at low volume and we're laying out the reasons and factors involved with such a question. And I find the science that someone like Wyn Palmer can add to be very interesting. That's also the reason things tend to get off topic and go to related issues.
 
The OP’s question could easily be formulated into a hypothesis. We could then use scientific method to prove / disprove it.

Or we could continue on this path ...

For the record, I’ve done it. All it requires is an A/B switchbox and the ability to match gain on both amps. Simple.
 
The OP’s question could easily be formulated into a hypothesis. We could then use scientific method to prove / disprove it.

Or we could continue on this path ...

For the record, I’ve done it. All it requires is an A/B switchbox and the ability to match gain on both amps. Simple.
What did you monitor and what results did you get?
 
MC240 vs bridged MC7270s ... same

Spectral DMA50 vs MC7270 ... same
What was the criteria of the test? Was it strictly listening, monitored distortion, etc? Were the speakers the same model with different coils or was it dummy loads? I agree with you, but I'm thinking your test may be lacking in supporting data.
 
What was the criteria of the test? Was it strictly listening, monitored distortion, etc? Were the speakers the same model with different coils or was it dummy loads? I agree with you, but I'm thinking your test may be lacking in supporting data.
Speakers were B&W DM 580

Preamp was a MC C29

Identical interconnects

Amps gain matched via a 1kHz test tone recorded at 0dB with a Fluke 87 DMM to a tenth of a volt

Volume control was not moved after gain matching

You were saying?
 
It’s the nature of this hobby to rebuke fact and cling to conjecture.

Oh, and how does one listen to dummy loads?
 
Speakers were B&W DM 580

Preamp was a MC C29

Identical interconnects

Amps gain matched via a 1kHz test tone recorded at 0dB with a Fluke 87 DMM to a tenth of a volt

Volume control was not moved after gain matching

You were saying?
It doesn't really tell me how you tested anything other than you set multiple amps to the same level. If you used only 1 set of speakers, how do you compare impedance? How did you determine the sonic quality? I'm assuming by ear. I'm not trying to pick on you, just trying to fully understand the test.
 
Also, using different amp designs(even of the same brand) doesn't necessarily mean it's the power capability of the amp that made a change if there is one.
 
It doesn't really tell me how you tested anything other than you set multiple amps to the same level. If you used only 1 set of speakers, how do you compare impedance? How did you determine the sonic quality? I'm assuming by ear. I'm not trying to pick on you, just trying to fully understand the test.
Myself, my buddy Mike, and my wife all took turns listening. Listener had the A/B switch in hand and could switch anytime they wanted to. Not one of us could tell any of the amps apart - at all, under any circumstances.

Cost me a steak dinner as Mike bet me that would be the outcome. Don’t believe me? Then set up a similar test in your space and report back. If more folks actually tested their hypothesis, it’d be a whole lot more difficult for marketing departments to write copy.
 
Myself, my buddy Mike, and my wife all took turns listening. Listener had the A/B switch in hand and could switch anytime they wanted to. Not one of us could tell any of the amps apart - at all, under any circumstances.

Cost me a steak dinner as Mike bet me that would be the outcome. Don’t believe me? Then set up a similar test in your space and report back. If more folks actually tested their hypothesis, it’d be a whole lot more difficult for marketing departments to write copy.
I already said I believe you, but I thought some details would be helpful. I was wondering so I could use any information in the future if I was to build or buy an amp, I could make a more informed decision on what's best. It was confusing because you came on here kind of implying we're morons for talking about the engineering aspect of amps and said it could be done scientifically. Then only mentioned an A/B switch. Which at first I thought it was referring to class AB. You could have just said set two amps to the same level and toggle between while listening. Not really that scientific, but is valid none the less.
 
Last edited:
I see what you mean now about limiting tweeter destruction, but I still don't see how it effects slew if it is not clipping.
Slew rate distortion occurs when some part of the amplifier is asked to change voltage at a rate which is greater than its ability to do so and hence it enters a non-linear region. To avoid that without changing the design of the amplifier one of two things can occur besides the trivial case of keeping the level low enough using the volume control- either the input signal is deliberately band limited using a built in low pass filter to avoid any possibility of the signal exceeding the rate - which would be a good idea with say, synthesized music, OR the input power spectrum is such that the rate of change is naturally limited- i.e. that the input signals are pink noise-like (1/f) with a built in upper bound, which is most like natural music, or red noise-like (rap music (a joke!)). Interestingly enough some sources (such as some MC cartridges for example) with substantial peaking either in the high sonic or supersonic regions can induce distortion as a result of their changing the 1/f characteristic of music at HF.
(Occasionally cartridges are loaded with minimal capacitance and high resistance and this can create ultrasonic resonant peaks of 30dB or more which can cause this, and other effects- caveat emptor!)
When testing opamps, for example, the way slew rate limiting is evaluated is to set the amp in a known gain configuration then drive the input with a very small rise time square wave that is just large enough to create slew rate limiting. Square waves have a Fourier series in which the terms are purely odd harmonic and decay at a rate which is 1/f^2 (i.e. the 3rd harmonic has amplitude 1/3 of the fundamental, the fifth is 1/5 etc.) so it approximates, if you will, infinite bandwidth music. If the square wave is low passed at say, 20kHz, then the rise time increases - although now overshoot exists due to the Gibbs Phenomenon. This is a reasonable proxy for a pink noise process with a built in, natural, bandwidth limitation.
If you test amps with this and not further overdrive the input then the slewing results can be different (more benign) than if the original wide bandwidth square wave is applied.
 
Last edited:
Hmmm...the suggestion I heard was that the smaller amplifier has the rise-time advantage - even when both amplifiers are driven to identical voltages.
Again, I cannot comment on how true this is, or even if. :idea:
It absolutely does not have to be that way, at least not at audio frequencies. It's harder to produce an amp which has extremely wide bandwidth (necessary for small risetimes) with no slew rate limiting as the output voltage increases, but not impossible. But, it certainly can be argued, beyond the point where the amp remains non-slew rate limited at all times both internally and externally, there is no purpose in having a smaller rise time and indeed there are negative aspects of such a design.
 
Slew rate distortion occurs when some part of the amplifier is asked to change voltage at a rate which is greater than its ability to do so and hence it enters a non-linear region. To avoid that without changing the design of the amplifier one of two things can occur besides the trivial case of keeping the level low enough using the volume control- either the input signal is deliberately band limited using a built in low pass filter to avoid any possibility of the signal exceeding the rate - which would be a good idea with say, synthesized music, OR the input power spectrum is such that the rate of change is naturally limited- i.e. that the input signals are pink noise-like (1/f) with a built in upper bound, which is most like natural music, or red noise-like (rap music (a joke!)). Interestingly enough some sources (such as some MC cartridges for example) with substantial peaking either in the high sonic or supersonic regions can induce distortion as a result of their changing the 1/f characteristic of music at HF.
(Occasionally cartridges are loaded with minimal capacitance and high resistance and this can create ultrasonic resonant peaks of 30dB or more which can cause this, and other effects- caveat emptor!)
When testing opamps, for example, the way slew rate limiting is evaluated is to set the amp in a known gain configuration then drive the input with a very small rise time square wave that is just large enough to create slew rate limiting. Square waves have a Fourier series in which the terms are purely odd harmonic and decay at a rate which is 1/f (i.e. the 3rd harmonic has amplitude 1/3 of the fundamental, the fifth is 1/5 etc.) so it approximates, if you will, infinite bandwidth music. If the square wave is low passed at say, 20kHz, then the rise time increases - although now overshoot exists due to the Gibbs Phenomenon. This is a reasonable proxy for a pink noise process with a built in, natural, bandwidth limitation.
If you test amps with this and not further overdrive the input then the slewing results can be different (more benign) than if the original wide bandwidth square wave is applied.
I understand how slew rate limiting limits frequencies above its capability. But it doesn't explain what you said about how having a HF and LF helps slew or saves tweeters. If you have an amp with a 100 volt max and you have a 40v HF on top of a 50v LF so that it is not clipping, and the HF is below the frequency the slew rate can produce, how is that different or easier on slew rate than if the 40v HF was produced on its own without the LF? Doesn't the amp have to keep up with the same rate of change whether it starts at zero or if it starts at 50v? The slew still has to be as fast for either scenario and wouldn't reduce the HF amplitude because it was used at the same time as a LF.
Or were you just referring to the frequencies contained in natural music and that the HF does not have the amplitude of the LF and that is what saves the tweeters?
 
The only help I can see a LF doing outside of reducing HF by clipping its power levels, would be if the HF was so close to the slew rate that it couldn't keep up if the HF had to start at zero which puts it in the slower rise area that is outside of the 10%-90% range.
 
If being able to double down into lower impedance speakers was the end all be all we should all be running pro amps, just sayin.

My little 35watt Kennys show that more power doesn't necessarily translate to better sound reproduction.
 
I understand how slew rate limiting limits frequencies above its capability. But it doesn't explain what you said about how having a HF and LF helps slew or saves tweeters. If you have an amp with a 100 volt max and you have a 40v HF on top of a 50v LF so that it is not clipping, and the HF is below the frequency the slew rate can produce, how is that different or easier on slew rate than if the 40v HF was produced on its own without the LF? Doesn't the amp have to keep up with the same rate of change whether it starts at zero or if it starts at 50v? The slew still has to be as fast for either scenario and wouldn't reduce the HF amplitude because it was used at the same time as a LF.
Or were you just referring to the frequencies contained in natural music and that the HF does not have the amplitude of the LF and that is what saves the tweeters?
Actually the 40v HF on its own is more benign than the 40v HF plus the 50v LF as the max rate of change will be equal to the sum of the max rates of change of both components (assuming they are not related in some way that prevents the maximum rates of change occurring simultaneously and in phase).
The issue is that in real live non electronic music you do not get high amplitude LF signals and high amplitude HF signals. Because of the 1/f nature if you have, say 80v at 100Hz you will only have 8v at 10kHz (100x the frequency, 1/100 the power, 1/10 the voltage for the same load impedance). That's why you need to have relatively very high power woofer and sub woofer amps mated with lower power mid range/tweeter amps.
 
Actually the 40v HF on its own is more benign than the 40v HF plus the 50v LF as the max rate of change will be equal to the sum of the max rates of change of both components (assuming they are not related in some way that prevents the maximum rates of change occurring simultaneously and in phase).
The issue is that in real live non electronic music you do not get high amplitude LF signals and high amplitude HF signals. Because of the 1/f nature if you have, say 80v at 100Hz you will only have 8v at 10kHz (100x the frequency, 1/100 the power, 1/10 the voltage for the same load impedance). That's why you need to have relatively very high power woofer and sub woofer amps mated with lower power mid range/tweeter amps.
OK got it, we're on the same page now.
 
Back
Top Bottom