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#1 |
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diyAudio Member
Join Date: Feb 2003
Location: ..
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Walt Jung has long been an advocate of 2 op amp (or op amp + buffer) composite circuits and points out their advantages – check his web site; “Op amp Audio” series
Gerald Graeme has also advocated 2 op amp composite amplifier, with high loop gain from 2 pole responses – “Amplifier Applications of Op Amps” 1999 devotes a chapter to composite op amp circuits and their compensation This sim circuit topology is close to circuits I have built and I have verified that they can achieve measured 1KHz harmonic distortion (and 1KHz IMD from 1:1 10KHz + 11KHz) below my 160dB instrumentation limit ![]() Composite amplifiers can reduce active device contributions to audio frequency distortion to unmeasurable levels (1 V input, 20 KHz sim results: ) ![]() The output op amp is a modified integrator that provides large audio frequency gain, those in the know will object that the loop phase response, which exceeds 180 degrees around 100 KHz invites oscillation or poor recovery from clipping ![]() (the Loop Gain Probe is available from the LtSpice Yahoo group files area - just cut it out and delete .prams lines if you don't want to use it) The clipping response is greatly improved by the symmetrical clamping diode bridge that holds the input op amp to +/- 1 V output when the output op amp saturates, this means that the input op amp is held in its linear operating region, its contribution to loop gain and phase shift is minimized, and its output only has to slew ~ 1V to when recovering from saturation ((1.6 V @ 20 KHz input, V(n005) is Lt1022 output) ![]() Simple back-to-back diodes would also provide for the improved clipping response, but the bridge reduces diode capacitance and nonlinear conduction current that add directly to the feedback error voltage and cause nonlinear distortion (distortion and phase margin # may be off slightly, I plotted those with all 1N418 diodes before it occurred to me to reduce clamp voltage with Schottkys, this means diode feedthru may be slightly higher due to higher capacitance form lower reverse bias on D1,2) |
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#2 | |
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diyAudio Member
Join Date: Feb 2003
Location: ..
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I thought I might collect some of these multiloop/gain boosted composite op amp ideas, this thread is already here...
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#3 |
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diyAudio Member
Join Date: Feb 2003
Location: ..
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over at headfi I'm encouraging the use of a multiloop topology with the TPA6120 (= THS6012)
posting here with the asc for those wanting to play with LtSpice
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#4 |
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Account Disabled
Join Date: Jun 2004
Location: Animal farm
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Good stuff jcx...Cheers!
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#5 |
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diyAudio Member
Join Date: Sep 2002
Location: Sweden
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Rod Elliott used to have an article at his site with a headphone amp consisting of a VFB + CFB combo. It was never a build project, but something he did to try out some samples of CFB ADSL drivers he had got. Unfortunately, that article seems not to be around anymore, and he now uses only the CFB amps as they are. Anyway, as far as I remember, his idea with the combo was to get the precision of VFB combined with the speed of CFB, and he said then it was the best headphone amp he had heard. I don't remember the details, whether there was any local feedback around each op amp, for instance.
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#6 |
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diyAudio Member
Join Date: May 2001
Location: Bangalore, India
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Elektor carried an article using VFB+CFB to make a very fast Composite Opamp. It was a concise article plus schematic by T.Giesberts.
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Sam |
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#7 | |
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diyAudio Member
Join Date: Jun 2004
Location: Oregon
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Quote:
I'd like to use the Loop Gain Probe. I downloaded it from the LtSpice yahoo group. Using your circuit, I set .param prb=-1 and ran it. No errors in the transient analysis with .asc and .asy files in their proper place. I then did an AC analysis run and I can get a plot of Vout in magnitude and phase. it looks flat out to ~300Khz. How do I tell LtSpice to show a plot of loop gain in magnitude and phase? Thanks, Mike |
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#8 |
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diyAudio Member
Join Date: Feb 2003
Location: ..
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the loop gain probe uses both V and I sources to test return difference which gives the correct result anywhere in the feedback loop - the usual simplified test with just a V source works best when the impedances are mismatched by the largest amount possible so that information/energy transfer is well approximated as flowing in one direction only
to use the loop gain probe you have to run 2 analysis, as in the commented out .step in the example above, then the correct value for the loop transmission (Bode's T commonly (and sometimes approximately) "return difference", “return ratio”, “loop gain”, ”excess gain”, “feedback factor”) is given by the complicated expression at the top of the sheet, you have to copy that into the plot as the trace definition you want to display (clik on the expression, copy its text, then go to plot>add trace and paste the expression at bottom of the box) I don't know where all of the Spice syntax for that expression is documented - the @1, @2 suffixes refer to the trace "steps" - the multiple passes of sim caused by the .step command Loop Gain probe theory: http://www.thekunderts.net/ken/docs/c&d2001-01.pdf https://www.eecs.berkeley.edu/~boser...%20lecture.pdf middlebrook paper: http://www2.enel.ucalgary.ca/People/Haslett/Jwhgrad.htm |
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#9 | |
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diyAudio Member
Join Date: Jun 2004
Location: Oregon
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Quote:
I cut and pasted the expression: 1/(1-1/(2*(I(V :i)@1*V(p:x)@2-V(p:x)@1*I(V :i)@2)+V(p:x)@1+I(V :i)@2))(note: is actually the text chars colon followed by p)and LtSpice complains about unknown current requested: I(V :i)so I found a .plt file that had this expression: 1/(1-1/(2*(I(Xp:Vi)@1*V(Xp:x)@2-V(Xp:x)@1*I(Xp:Vi)@2)+V(Xp:x)@1+I(Xp:Vi)@2)) and I cut and pasted this expression and was able to get it to work. It duplicated your results. Looks like the names used in the loop probe changed or something. Thanks for the help, Mike |
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#10 |
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diyAudio Member
Join Date: Feb 2003
Location: ..
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I grabbed Bob's example sim from the TPC/TMC debate in the Cordell Book thread Bob Cordell's Power amplifier book
my poking at it seems to indicate that the distortion is limited by the slow output Q and simply can't be made much better by feedback - especially the THD 20KHz that Bob likes as a simple quality metric (at least without going deep into conditional stability territory with 3-rd order or higher loop gain schemes) if you can't fix up a amp with more feedback then the other tool is Black's Error Feedforward - rare in audio because of the difficulties power output combiner but famous none the less due to Quad’s "Current Dumping" amplifier a error feedforward amp is defined by having 2 independent power amp paths to control the output - and the consequent difficulty of combining the outputs without their mutual loading causing unwanted additional (destabilizing) feedback The VanderKooy Lipshitz Error Feedforward paper http://quad405.com/jaes.pdf shows several schemes - "Current Dumping" actually wraps negative feedback around the "dumper" amp stage - but 2 other schemes are shown - I chose the Parallel Feedforward from their fig 4b - which doesn't intentionally add loop feedback to the main amp and the coupling through the output impedances of the amps is minimal when used with a frequency selective power combiner so the following is a Composite Amp using a large, slow discrete amp and a fast error feedforward op amp path the instrumentation op amp measures the error at the diff pair input of the main amp with a gain of 10x, and then the CFA DSL driver op amp integrator provides the required error correction V drive for the Resistive leg of the L,R power output combiner network Bob's THD 20KHz number is improved by ~20x in this sim you will need Bob's zip file and to put my asc in the same folder with Bob's Cordell Models.txt file or you can download Bob's transistor models from his book's site Last edited by jcx; 30th December 2010 at 09:50 PM. |
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