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Part of the beauty of some (primarily lower power and often single ended) class A amps is the simplicity of their circuitry. I think simpler circuitry often translates to better sound. Once you start getting into higher power amps, the circuitry gets more complex, and this is where I think the playing field evens out a bit to varying degrees (in terms of sound quality, distortion characteristics, etc. etc. of the different amp classes). It's all a system of trade-offs and figuring out what you enjoy listening to / what type of speaker suits your tastes, and finding a suitable amp for your sound / speaker choice.
No doubt we find instances where poorly designed and implemented complex ccts result in poor sound. But the same holds true of simple designs which can also be poorly designed and implemented.But what of those ccts which are neither poorly designed nor poorly implemented? For argument sake. We have 2 amps. One is a very powerful and complex class AB amp. The other is a very simple, class A amp. Let’s presume we hook up each of the amps to appropriate speakers, using appropriate speaker cable in appropriate rooms and play music such that neither enters, nor approaches, clipping levels. We properly measure the 2 amps to see how they are performing under such conditions.Let’s say the powerful and complex amp is measured and is shown to perform with no audible errors in distortion, noise and frequency response. The same is true of the simpler amp. Effectively all both amps do to the inputted voltage signal is increase it by x amount of gain. Nothing more, nothing less. If both amps are shown to add gain with no audible levels of distortion then does it really matter what cct topology they employed in order to arrive at that gain figure since both amps will sound like each other (ie like nothing)?
I would like to point out as I have previously that the things that have to be done in high power amps. Current limiters, reduced bias and high voltage swings can cause problems into various loads. Low power amps do not usually have limiters as they don't need them. I will go so far as to say the low voltage high current amplifiers have a far better chance of sounding better on a variety of loads than high power amps when used in their voltage range. When you exceed 25 volt rails on a bipolar transistor amp you start to need limiters for short circuit protection. Anyone care to say what power you get from 25 volt rails at 8 ohms? What happens at 50 volt rails?I have experienced the problems of high power amps with many speakers. There are speakers where I had to put a 1 or 2 ohm resistor in series to get the limiters to stop cutting in. Of course that reduced the damping markedly so I am not saying that is a solution except in a pinch. At least the 250 watt amp stopped clipping at low power.I think people have to know more about the problems encountered in high power amps. That is the point of my entering this discussion. I also think most people here find that amps sound like something.
Roger, indeed, one may encounter issues if the amp isn't up to the job asked of it.Answers, presuming RMS values, ~78w and 312w.
No. And that's the point I was trying to make.However, we all know design and topology affect sound..........unless you believe all amps sound the same.With that said, I think simple class A circuit (single ended particularly) may always have an advantage in terms of being more transparent to the source (due to less circuitry). I'm not talking about just distortion figures, I'm talking about signal preservation through the electronic chain. But, having said that, there's no way to currently design a practical single ended class A amp that is also higher powered. So that's where well designed class A/B has a major advantage. While one amp may be more transparent, it may not have enough power for a broad range of applications. The other approach may be less transparent, but has more power and is more practical (in general). It's more of an apples vs oranges discussion than an Fuji apples vs Gala apples discussion. Apples and oranges are both good. It just depends on what you're hungry for. One wouldn't eat an orange if he/she was wanting / expecting it to taste like an apple. Know what I mean?
How does one determine if the amp is up to the job? What are the parameters you suggest to check?Answers, RMS power 25 watts for 25 volt rails, 100 watts for 50 volt rails. These are the numbers found in practical amplifiers.
The only surefire way to know is to measure it ... hooked up to your speakers, with your chosen speaker cables, in your room and playing the most dynamic music you'll play at the highest volume level you figure you'll listen at. I realize this isn't practical for most. But is for some. I was listing the maximum power ratings attainable for a CVS amp based on P=E^2/R.
Plenty of good discussion. Here's my take on slew rates and TIM.The argument is that large amounts of NFB results in slew rate limiting which ends up in increased amounts of TIM. So, if NFB is lowered we wouldn’t see slew limiting nor increased levels of TIM. Those who argue against such a claim suggest that it is not the level of feedback that imparts slew rate limiting and the resultant TIM but, rather, it is improperly implemented circuits done with excessive compensation that is the real cause. AFAIK, there is no peer reviewed evidence that audible levels of TIM exists in properly conceived gear. As for slew rate. Slew rate indicates the slope (steepness) of the wave the amp can produce and is just a handy way of combining amplifier power (voltage) and frequency response into a single, convenient, value. It’s specified as a change of voltage over a specific period of time. This single value is not really needed as you can get more meaningful info by looking at the amps power (voltage) and its high frequency response limit. But we like convenience it seems ….. even at the cost of inaccuracies. By example. For an amp to produce 15v at 1 Hz, its output voltage would need to slew at a rate of 15v/second. So, a very shallow slope if viewed on a scope. By contrast, if the voltage was increased tenfold to 150v, the slew rate would need to be 10 times faster or, in this case, 150v/second. And the slope would be 10 times steeper. If the frequency is raised from 1 Hz to, say, 10kHz, the slew rate would rise by a factor of 10k and we now get 1,500,000v/sec (or, since # is getting very large and unmanageable, expressed as v/uS instead). For an amp that outputs 150v and has a linear high frequency response of 100kHz (as is the case with most SS amps these days), the slew rate would be 150v/uS. We know that output voltage determine power so lower powered amps will have smaller slew rates than higher powered amps … at the same frequency. Also, amps that have lower frequency response will have lower slew rates than amps that have higher frequency response. But, we also have seen that an amp that is spec’d out with a very high frequency response (ie 100kHz) will result in a large slew rate. But, us humans can’t hear above 20kHz so, in this case, the amp that goes to 100kHz won’t sound any different but, for a given power, it will have a slew rate that is 5x higher than that of the amp that is rated for 20kHz. And, you can almost bet that it’ll be deceitfully marketed as such. Thus the inaccuracy noted above.It all can be confusing. Just note that, while slew rate must be high enough, a high slew rate, in and of itself alone, might not define the sound of an amp. Since all quality amps linearly produce 20kHz, it really is the voltage (power) that makes the difference when it comes to slew rates.
Sorry, constant voltage source for the acronym. I agree on the practicals. Yes, I scope test as well. I am curious. Do you believe that current measurement techniques fully and adequately describe human hearing? Further, do you believe the general consensus on the distortion threshold of human hearing (as I described previously), is accurate?
Hi, I was looking over some of your numbers today and wanted to see if you agree with some corrections. I kept you whole quote intact as I also don't agree with the first statement but do agree with the second. Excessive compensation is the issue not the amount of feedback.
I don't know why you started with a time period of 1 second but no matter. When you convert 1,500,000 volts per second to volts/microsecond the correct answer is 1.5 V/us. Raising the frequency from 10KHZ to 100 KHZ as in your example makes the slew rate 15 v/us, not 150.
The frequency response (usually stated at low levels of a watt) is independent of the slew rate. You can make an amp with very wide bandwidth that has a very poor slew rate. This is why slew rate became important.
Thanks for the acronym, keep in mind that few people will know them. Its fine to use it once defined in each post.
I do not believe measurements fully describe amplifiers as we hear them. However if all the tests are done, and there are many that are not, we do get a lot closer to what makes a good amplifier. One should pay attention to John Atkinson's measurements of frequency response alterations with a speaker load. It's the first graph he publishes in every amp measurement. Perhaps that is because he finds it most important also.
What I try to get listeners to understand is when amplifier A has some very measurable differences from amplifier B then we might want to consider how those differences influence what we hear. The very first big difference is damping, which is often ignored. Damping factors vary widely from amp to amp and their effect varies from speaker to speaker.I would suggest a simple test. When two amplifiers are being compared, hopefully in an A/B test, make the amp with the higher damping factor equal that of the lower by adding a high quality resistor to make the damping factors equal. This resistor will usually be less than an ohm and not cause any significant loss of power. Now we have leveled the playing field to the point where other characteristics can be studied. If it turns out that someone likes the sound of a low damping amplifier on his particular speaker and has a high damping amplifier, wouldn't it be nice to make that change with a resistor rather than a whole new amplifier?
I do not believe measurements fully describe amplifiers as we hear them. However if all the tests are done, and there are many that are not, we do get a lot closer to what makes a good amplifier. One should pay attention to John Atkinson's measurements of frequency response alterations with a speaker load. It's the first graph he publishes in every amp measurement. Perhaps that is because he finds it most important also. What I try to get listeners to understand is when amplifier A has some very measurable differences from amplifier B then we might want to consider how those differences influence what we hear. The very first big difference is damping, which is often ignored. Damping factors vary widely from amp to amp and their effect varies from speaker to speaker.I would suggest a simple test. When two amplifiers are being compared, hopefully in an A/B test, make the amp with the higher damping factor equal that of the lower by adding a high quality resistor to make the damping factors equal. This resistor will usually be less than an ohm and not cause any significant loss of power. Now we have leveled the playing field to the point where other characteristics can be studied. If it turns out that someone likes the sound of a low damping amplifier on his particular speaker and has a high damping amplifier, wouldn't it be nice to make that change with a resistor rather than a whole new amplifier?
Keep in mind that voltage alone has no power. You need current too. Power is voltage x current. On another note for low power vs high power amps. I just thought of this analogy for the low power crowd.When you want to get a lot of water through a hose and you are only a few feet from the spigot, doesn't a 15 ft hose provide a lot more water flow and power than a 100 ft hose? Does at my house. Taking that analogy further, what is power in water? Isn't it flow x pressure?
Bob Carver kind of did just that with some of his Sunfine amps. He had a "voltage connection" and a "current connection". The current connection would attempt to mimic the tube sound by a resistor in line to vary the load seen by the amp, and thus change the load impedance.I do think there are measurements that could capture performance better. A spectrum analyzer could provide much more information about the amp interaction with a given speaker load. The current measurements of a a set of various single frequencies into a load resistor may help tell ho stable it is, but not much about the sound.
My prof explained it to me this way many moons ago. Voltage is the "pressure" that pushes electrons through a conductor while current is the "flow" of electrons. Power is the product of them.