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OPA1656: High-Performance CMOS Audio Op Amp

I was assuming that we take 20kHz as the highest frequency to expect to reproduce. At 20kHz and the highest amplitude is where the signal has the highest slew rate.
SR = 2*pi*f*Vpk. Do the math.
Then the rule of thumb: take 2x to 4x that for safety. What's so hard to understand?Jan
OK. Slew Rate = 2 x π x 20,000 (Hz) x 28 volts (peak) = 3,518,583.772 times 4 for safety = 14,074,335.09
Huh?
 
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OK. Slew Rate = 2 x π x 20,000 (Hz) x 28 volts (peak) = 3,518,583.772 times 4 for safety = 14,074,335.09
Huh?

You've quoted a peak value of 28V which is actually the peak to peak. So your final number is too high by a factor of two. Actually it isn't even that. The OP1656 will swing within 0.25V of the rails, so for +/-18V it will do 17.75V. So your equation should give 8.5V/us even with a factor of 4 for safety.

As compared with the OPA1656 which is 24V/us.

The question is rather moot anyway. There is no practical audio program material which will have 24dBu (which is what 17.75V peak corresponds to) at 20kHz.

The applications that slew rate limiting is important to take into account is using the device in non-audio applications.

Craig
 
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And I would bet that the amplitude of each step is too small to actually reach the slew rate of the amplifier. Remember, to actually hit the specified slew rate of an op amp, you have to create a large enough voltage between the op amp inputs to direct 100% of the tail current into the compensation capacitor. Just because you have a fast edge doesn't matter. You can put a 1mV square wave with an infinitely fast edge into an op amp all day and never exercise its slew rate. It will remain in small signal operation where its rise time probably 0.35 / bandwidth (single pole system).

Here is my frustration with the slew rate conversation around op amps. I think what we really need for audio op amps, is not necessarily high slew rate but rather linear input stages. What I mean by linear input stages is ones that have minimal variation in their transconductance for a wide range of input differential voltages.

It USED to be true that an op amp's slew rate was a fairly good indicator of input stage linearity. Op amp manufacturers would degenerate the input pair and so they could stabilize the op amp with a much smaller compensation capacitor, and the resulting slew rate of the op amp (determined by tail current and comp cap size) was much higher. This is why older high speed op amps and amplifiers targeting video applications have fairly high broadband noise, it is thermal noise from the degeneration resistors.

But all sorts of nonlinear circuits are also now commonly used to increase an op amp's slew rate. These "slew boosting" circuits detect large differential voltages at the op amp inputs, and then dump extra current into the LTP to increase the slew rate during the transient. This is kinda like putting nitrous oxide on a honda civic. You get civic gas mileage (power supply current) during regular usage and all that extra slew rate in a drag race (large square wave with a fast edge). But, depending on how the slew boosting circuit was implemented, this could have drastically reduced the linearity of the input stage. In fact it can even introduce discontinuities into the gm vs Vdif curve.

I'm not anti slew-boost, in fact I have seen it done extremely elegantly to improve the input stage linearity (OPA1692 is an example of this). But I have the luxury of seeing this as an insider, as the customer you have no way of knowing how the datasheet slew rate spec was achieved unless it is so drastic that it shows up in THD curves.

So where does that leave us? For me, beyond a certain threshold, more slew rate is pointless and taken to the extreme it actually makes me skeptical of an amplifier's linearity because I don't know what deal was made with the devil to get all those slew rate bragging rights. It could have a totally non-linear input stage, or an architecture that is going to show low frequency distortion from thermal feedback effects (Class-AB or H-bridge input stages). What is that threshold? A reasonable rule of thumb would be 6 to 10 times the slew rate of the maximum sinusoidal frequency and amplitude expected, e.g. 10 * 2 * pi * f * A.


Very nice info, thanks john! So having all that said, what's the best suited TI opamp for an I/V then? ANd what about the fully differential ones, what are the implications of using these for a differential I/V?
 
Thx you John , it makes a lot of sense ..


I was using a bipolar opamp with good slew rate and linear input stage... I assumed that I heard the better slew rate , now I understand that it was the linear input stage. (they are advertised as having linear input stage up to a few mV)

TI has OPA1656 and OPA2156 jfets that will work nicely for IV stage (while having low voltage noise)
 
Very nice info, thanks john! So having all that said, what's the best suited TI opamp for an I/V then? ANd what about the fully differential ones, what are the implications of using these for a differential I/V?

I always try to maximize the gain in the I/V stage of a DAC output. This is because the signal gain is directly related to the value of the feedback resistor, but the noise in the broadband region is usually determined by the feedback resistors thermal noise, proportional to its square root. That means there is an SNR benefit to maximizing gain. Plus its the first stage in the circuit, and you should maximize gain at this point anymore. So how do we pick an op amp?

You're looking for an op amp with a combination of voltage and current noise that provides the best noise performance at that particular source impedance (parallel combination of the DAC output impedance and the feedback resistor). If that impedance is <1kOhm, I would look at BJT input devices. >10kOhm? No brainer there, JFET and CMOS types. What about the murky world of source impedances between 1-10kOhm where it seems like every audio circuit ends up?! Here there are a number of options: BJT-inputs without bias current cancellation (OPA1622), Super-Beta BJTs (OPA2210), Low voltage noise JFET and CMOS (OPA1642, OPA827, OPA828, OPA1656/2156).

Of course there are a number of other factors to consider, like the ability to drive the input impedance of the following circuitry with low distortion levels. But I personally start with noise. Although I have seen plenty of debates on here about whether distortion sounds bad or good, I have never seen anyone argue that noise sounds good.

On the topic of fully differential amplifiers (FDAs): while at first glance this might seem like a great idea, it's important to note that the common mode voltage at an FDA's inputs is a function of the output common mode voltage, and the input signal. Usually current output DAC performance depends heavily on maintaining the proper voltage at the DAC output and that is not as straightforward on an FDA as it is with an op amp I/V stage. Its certainly something that a number of people have explored though.
 
I always try to maximize the gain in the I/V stage of a DAC output. This is because the signal gain is directly related to the value of the feedback resistor, but the noise in the broadband region is usually determined by the feedback resistors thermal noise, proportional to its square root. That means there is an SNR benefit to maximizing gain. Plus its the first stage in the circuit, and you should maximize gain at this point anymore.

OK, by maximizing gain you mean to increase the I/V resistor as far as possible, i.e. to achieve as big an output voltage one can handle in the following stages?

So how do we pick an op amp?

You're looking for an op amp with a combination of voltage and current noise that provides the best noise performance at that particular source impedance (parallel combination of the DAC output impedance and the feedback resistor). If that impedance is <1kOhm, I would look at BJT input devices. >10kOhm? No brainer there, JFET and CMOS types. What about the murky world of source impedances between 1-10kOhm where it seems like every audio circuit ends up?! Here there are a number of options: BJT-inputs without bias current cancellation (OPA1622), Super-Beta BJTs (OPA2210), Low voltage noise JFET and CMOS (OPA1642, OPA827, OPA828, OPA1656/2156).

Of course there are a number of other factors to consider, like the ability to drive the input impedance of the following circuitry with low distortion levels. But I personally start with noise. Although I have seen plenty of debates on here about whether distortion sounds bad or good, I have never seen anyone argue that noise sounds good.

Ok, given the example I have at hand, the ES9038Q2M in mono mode: Output resistance of the DAC itself with both outputs parallelled is around 400Ohms which clearly falls into category one. BJT it is then. Any recommendations on this front? I guess the widely used OPA161(1|2) would be one of them?

On the topic of fully differential amplifiers (FDAs): while at first glance this might seem like a great idea, it's important to note that the common mode voltage at an FDA's inputs is a function of the output common mode voltage, and the input signal. Usually current output DAC performance depends heavily on maintaining the proper voltage at the DAC output and that is not as straightforward on an FDA as it is with an op amp I/V stage. Its certainly something that a number of people have explored though.

This topic is a bit wierd regarding ESS DACs. Most peoply seem to adjust the voltage at the noninverting terminal of the I/V opamp so that it will output 0V in reference to GND. This will lead to a DC voltage of less than 1/2 AVCC at the output pins of the DAC, which in turn doesn't seem to bother it at all. Will have to test this. Or are you not talking about DC here? What's your opinion on wether this should make any noticeable difference at all, having the I/V outputs sitting at 0V or higher - with parts that have such little distortion the DC operating point shouldn't really matter, should it?
 
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Paid Member
Stuart Yaniger (SY here) and I have visited Johnc124 last Friday in Tucson. In all the discussions it became clear that they have a lot of great audio parts coming out. Won't steal his thunder, but John clearly has diyaudio at heart. You will be pleasantly surprised.

Also received a small parting gift of about 50,000 OPA1656's. Each ;-)

Jan
 
Stuart Yaniger (SY here) and I have visited Johnc124 last Friday in Tucson. In all the discussions it became clear that they have a lot of great audio parts coming out. Won't steal his thunder, but John clearly has diyaudio at heart. You will be pleasantly surprised.

Also received a small parting gift of about 50,000 OPA1656's. Each ;-)

Jan

It was great having you guys visit! You'll have to come back for another tour when our new facility is finished.
 
So how do we pick an op amp? You're looking for an op amp with a combination of voltage and current noise that provides the best noise performance at that particular source impedance (parallel combination of the DAC output impedance and the feedback resistor)........What about the murky world of source impedances between 1-10kOhm where it seems like every audio circuit ends up?! Here there are a number of options: BJT-inputs without bias current cancellation (OPA1622), Super-Beta BJTs (OPA2210), Low voltage noise JFET and CMOS (OPA1642, OPA827, OPA828, OPA1656/2156).
Yes, indeed---all very good opamps!! BUT...the almighty $$$$$$:
OPA1622 $5.73 OPA2210 $5.17 OPA1642 $2.08 OPA827 $10.80 OPA828 $7.54 OPA1656 $2.72 OPA2156 $2.91
 
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Yes, indeed---all very good opamps!! BUT...the almighty $$$$$$:
OPA1622 $5.73 OPA2210 $5.17 OPA1642 $2.08 OPA827 $10.80 OPA828 $7.54 OPA1656 $2.72 OPA2156 $2.91

That's with the aim of performance. On the other hand you can go to Analog Devices and get much more expensive opamps with about as good or worse performance.
If price is your concern, get some 5534 or perhaps njm8068 njm4585.
Also pricing for 1000+ isn't really that expensive for opa1656, opa1602, opa1612.