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Slew Rate in Audio Amplifiers - What Does it Mean?

by February 08, 2013
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Slew Rate Measurement

Slew Rate Measurement

Ever wonder what slew rate was all about? No, it has nothing to do with how a drunk person slurs their speech. This article gets to the basics of Amplifier Slew rate and what it means.

When reviewing the spec sheet of an amplifier, one potentially unfamiliar term you may run into is slew rate.  There are a lot of gobbledygook explanations floating around the web which seem to misunderstand the basic premise, so we at Audioholics are here to clear the air. In short, slew rate has little to do with how an amplifier produces dynamics so much as its ability to effectively maintain output into higher frequencies.  It is the rate of how quickly an amplifier can respond to a rapid change of input level.  This is measured as a change in voltage with respect to time as can be seen in the main image of this article.

Digging Deeper

The first thing that people tend to see in slew rate specification is that it is measured in volts/microsecond or v/usec. From there, people jump to the conclusion that an amplifier with a higher slew rate is more responsive, dynamic, etc. Since a picture is worth a thousand words, let’s take a look at a relatively simple graphic.

Sine Wave

Depicted above are sine waves of various frequencies; the lowest frequency is on top followed by sine waves of progressively higher frequency. You’ll notice that as you go up in frequency, the value of the sine wave changes at a greater rate than at lower frequencies: this is what slew rate is all about. Simply, slew rate tells us how high in frequency an amplifier can play for a given voltage level.

So now that we know what it is, how much slew rate is enough? The basic formula to obtain a minimum necessary slew rate for an amplifier is:

 Slew Rate = 2 x π x Frequency x Peak Voltage

As you’ll note, the factors we need to fill in are how high in frequency we want to go and how much output, as measured in volts, we want to achieve.

So as a real world example, what is the bare minimum slew rate we need to effectively achieve THX Select 2 certification, which calls for peaks of up to 50V on all channels? Well, first we need to select a frequency to base our calculation on; 20kHz would seem a good starting point, as this is the generally accepted upper limit of human hearing. Plugging those numbers in, you’ll find that a THX Select 2 amplifier should have a slew rate of no less than ~6.3V/usec if it aims to achieve full output at 20kHz. 

Most well designed amplifiers are flat out to 100kHz so in that case you would need a minimum slew rate of about 32V/usec in order to achieve such a wide bandwidth.

At this point, an observer may note that the number calculated above is a lot lower than the specifications you are likely to encounter, even on entry level receivers. As an example, the Harman Kardon AVR 1565 boasts a slew rate of 40V/usec. Considering its rated power of 70W per channel into 8 ohms (the above example of 50V translates into a 312.5 watt peak at 8 ohms), 40V/microsecond would appear to be gross overkill. Realistically, it is a matter of good engineering. The bare minimum that we’re calculating is just that; most good linear amplifiers aim for flat response well beyond 20kHz, not because we can hear that high or because we have loudspeakers capable of reproducing such frequencies effectively, but to ensure slew rate related problems are a total non-issue within the audible band. Simply put, once you start tossing in other requirements, i.e. expecting practically zero distortion even at full power into a difficult load at 20kHz (a problem area for some amplifiers, notably Class D), a bit of extra margin in terms of slew rate can come in quite handy.

With all this in mind, what are the real world consequences of a marginal slew rate? This question is a bit more difficult to answer, as a lot depends on the source material. It should be pointed out that unlike laboratory conditions, most people aren’t running 20kHz sine waves through their systems at full output; real world material typically has little energy in the top octave (10kHz-20kHz), which can help mask the effects of a marginal slew rate. Odds are in and of itself, slew rate is unlikely to be a limiting factor in an amplifier’s real world performance; of course as mentioned above, if you’re expecting practically perfect performance under all circumstances, extra margin doesn’t hurt.

Editorial Note about Slew Rate from Sergiu Ignat – Electronics Designer for Classe

Slew Rate (SR) indeed expresses the ability of an amplifier to follow the input and as the formula implies this applies to the high frequencies within the passband of the amp. However most amplifiers have an input low pass filter used to minimize RF ingress and to limit slew rate induced distortions. Therefore even if the intrinsic SR of a power amp can be higher most designs tend to limit the bandwidth of the applied signal and in consequence the real SR may be lower than the one specified. If a manufacturer specifies “SR measured with input filter disabled” then it is the real deal.

By itself SR is a second order specification, not all manufacturers publish/measure it and is not indicative of sound quality if not accompanied by distortion numbers at the frequency of interest. For example an amplifier can follow a square wave at 20 kHz very closely in terms of rise/fall times, which in turn will give a very good SR number but if it does so with 20% overshoot and/or with long settling times (ringing that lasts for most of the pulse duration)…then the amplifier is probably not very good sonically (it has a hot and seemingly “detailed” top end).

The formula can be rewritten as: SR=2*π*f*√(2*P*Z)

This shows that if you need to deliver the same power at the same frequency into a higher load you need a higher SR. Considering the impedance swings of real world speakers we can see why having a healthy SR is not a bad idea as long as distortion and other parameters are kept in check.

On the other hand nobody expects a power amp to deliver full power at say 200kHz, the filter capacitors in the supply may not be able to sustain that kind of ripple current.

Classe CA-2300

Classe CA-2300 Amplifier Internal View

In our detailed review of the Classe CT-2300, we measured impeccable performance in every aspect.  The amplifier was wide bandwdith, low distortion and very capable of driving low impedance loads at high sustained outputs.  This amplifier exhibited no slew rate induced problems.

Conclusion

By now you the reader should understand that slew rate has precious little to do with the dynamics or punchiness of an amplifier, although one can imply that a more powerful amplifier requires a higher slew rate. Slew rate is all about effective bandwidth. Further, you’ll find that you don’t necessarily need a top echelon amplifier to extend useful bandwidth well beyond 20kHz. Presuming Harman Kardon isn’t fudging their specs too badly, the slew rate of the entry level AVR 1565 is sufficient to give it full power output to 100kHz and beyond, which even a conservative engineer would consider (in a dry tone) “adequate”. Of course, now equipped with the knowledge of how slew rate and bandwidth are intertwined, you too can see just how true some claims of bandwidth out to 300kHz and beyond really are. Happy listening (and calculating)!

 

About the author:
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Steve Munz is a “different” addition to Audioholics’ stable of contributors in that he is neither an engineer like Gene, nor has he worked in the industry like Cliff. In fact, Steve’s day job is network administration and accounting.

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