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#1 |
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diyAudio Member
Join Date: Aug 2004
Location: Behind you
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Having recently been considering class AB input stages, I wondered how it might be possible to reduce the added complexity of multiple current sources that the long tail pair type often use. One possibility is to use the LTPs' own current mirrors as current sources.
Now, class AB LTP input stages are symmetrical, so you can't just put current sources in them because the VAS quiescent current becomes undefined. So the first thing to do is apply some current feedback from the VAS. This yields the circuit on the left in the attached picture. Changing this to class AB yields the circuit on the left. The LTPs are connected at the tails and their tail current sources removed so that each LTP provides the current for the other, and the bases are biased on with diodes. The current can increase past the quiescent current, hence the class B part. The constant currents that feed the diodes are simply provided by adding extra outputs from the current mirrors (Q9/11/13/14). Note that the emitter resistors for these extra current source transistors can be larger than those in the main current mirror to reduce the current through the diodes, for efficiency (Widlar current mirror). It would also be possible to use a "diamond buffer" arrangement to provide the bias voltage instead of diodes, giving higher input impedance. The whole point of class AB input stages is to increase slew rate, so I simulated that and got 60V/us, compared to 30V/us for the class A version. This is with relatively large 100pF Miller compensation capacitors, LTP tail current at 4.7mA (I1 and I2 in the class A circuit, the current through R5 in the class AB circuit) and VAS current also at a conservative 4.7mA. GBP, phase margin and distortion are all approximately the same for both circuits, so the main compromise is between slew rate and complexity. Higher slew rates would be possible by increasing LTP current and decreasing the value of R5 and/or the emitter degeneration resistors (which are inextricably linked to the quiescent current, unless the bias scheme is changed). Insanely high slew rates are possible. So what do you do with all this slew rate? I dunno, but it's interesting anyway. Note that the capacitors C3/4 were needed to prevent overshoot in the sims, but might not be needed in a real circuit. EDIT: The image was too big, so I chopped the supply voltages off.
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#2 |
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diyAudio Member
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Good work!
Here is what I used when wanted as simple as possible complementary class A opamp with gain = 1. A first, I replaced transistors in current mirrors by diodes. Second, I replaced transistors in LTP pairs by diodes. And third, I used resistors in tails so currents depend on voltage. LTP currents were adjusted by resistors in tails to get no more than max needed current swing on the real output load, so in case of accidentally lower load resistance it protected itself limiting the current. Surprisingly, the sound was vacuum tube-like!
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The devil is not so terrible as his mathematical model! Wavebourn: We Create Creativity! |
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#3 |
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Banned
Join Date: Apr 2003
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Just curious - have you seen the class AB input stage from the Smith, Koen and Witulski paper? I think that paper is on OS's site. Here's a pic.
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#4 | |
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Account disabled at member's request
Join Date: Aug 2005
Location: Toronto
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#5 |
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diyAudio Member
Join Date: Dec 2007
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I designed a high-performance opamp for driving low-Z headphones (50R and under) a while back and have been refining it for a while. The idea was from the Smith et al paper referenced earlier (Figure 13, specifically). You might be interested in it. Performance is absolutely excellent (I have an AP 2722 to play with intermittently so I can get some real numbers).
It is fully class-AB, including the input stage, which is a dual diamond buffer arranged as a fully-differential V-to-I converter. A simple current-mirror gain stage slews a gang of output MOSFETs. All devices are TO-92; my stereo prototype is on a 4.5x4.5" protoboard along with a DC servo. The gate-drain capacitance of the FETs is enough to provide good compensation. It's picky about decoupling around the input stage, so the schematic is a pseudo-layout to show what is needed. Basic specs: * Unity gain bandwidth: 35MHz (measured; unity gain stable; 60 deg phase margin) * Open-loop bandwidth: ~4KHz (approx. 80db OLG) * Slew rate: 1000v/uS (!!!) (measured; 10v step on 24v rails) * THD/IMD: under -110dB (<20khz sine at around 2v into 50R), 2nd harmonic * Idle current: about 12mA for input and gain stages, output set at 20mA |
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#6 | |
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Banned
Join Date: Apr 2003
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#7 | ||
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diyAudio Member
Join Date: Aug 2004
Location: Behind you
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http://mrevil.pwp.blueyonder.co.uk/ |
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#8 | |
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Account disabled at member's request
Join Date: Aug 2005
Location: Toronto
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What would be the use of this configuration in the discrete world? We already have all the PNP's we need, beta, Ft, you name it. |
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Banned
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Account disabled at member's request
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Location: Toronto
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