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#211 | |
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diyAudio Member
Join Date: Sep 2006
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Quote:
Now, will it work in practice? Yes, but your mileage may vary. The crossquad is a pretty temperamental circuit, relying on a precisely controlled amount of positive feedback to function, and that feature plus the parasitics of real world circuits make an interesting mix... If you build the circuit exactly as on the schematic, it will probably oscillate like mad. If you try the usual recipes to tame the oscillations, like base stoppers and similar, not only will they not cure the problems, they will make them much worse: at the bases of the input transistors, a negative resistance of Re-e/Hfe is created. If that negative resistance is parallelled with a positive one (the source impedance) larger than itself, the resulting equivalent resistance is negative too, with results you can imagine. By adding base stoppers, you increase the source resistance, making the problem worse. And because the Hfe drops at high frequencies, input resistances much smaller than expected can cause problems. One solution is to bypass the base with a small value cap, to reduce the apparent impedance at high frequencies. That's just an example. There are a number of other mechanisms leading to oscillations. The compensations of the amplifier itself need to be adjusted, to take into account the effects of the Xquad in the overall loop. It is not a simple task, but it is doable. I have made functionning designs based on a crossquad (not in the Circlophone though). Some other pecularities have to be remembered: the phase is reversed compared to a standard LTP, but when it saturates, it degenerates and reverts to the normal phase. And it only takes several hundreds mV to saturate, however large is the tail current and/or the degeneration resistor. This leads to "interesting" behaviors... Which is why there are back to back schottkys at the input. If you surmount all those problems, the actual performance you can obtain will be strongly dependent on the matching of the transistors, but with low power devices, a good match is not difficult to achieve.
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#212 | |
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diyAudio Member
Join Date: Sep 2006
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Quote:
There is a variant of the cross-quad, created by Eva (I think so, I have never seen it elsewhere, and it is typical of the circuits she is capable of creating); it is better behaved than the 4 transistor version, but it doesn't deliver the raw performances of the naked Xquad. I named it the EvaQuad, but EvaHex might be more appropriate: Reinventing the N-channel wheel? A working example of a crossquad can be found in the voltage gain stage of the Tringlinator: The Tringlinator: a MOS-based Tringlotron amplifier But there, it is used with a well-defined gain of 7 rather than as a pure high gain block, making it rather less finicky. Note that the Tringlotron, the power stage of the Tringlinator is also a kind of vertically-stretched crossquad. All this explains the remarkable performances of the complete Tringlinator, despite the absence of GNFB.
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#213 |
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diyAudio Member
Join Date: Nov 2007
Location: Dallas
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So, you saying we just need DIACs to stopper the bases, right?
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#214 |
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diyAudio Member
Join Date: Nov 2007
Location: Dallas
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I been playin w. evquad (plus active tail) on sim.
This sems to me no different than a quad with a current mirror output instead of (or in parallel with) the standard outputs... Why is this one said to be any more stable? Sims OK, but all the same worries. |
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#215 | |
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diyAudio Member
Join Date: Sep 2006
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Quote:
Look at the first pic: with an input of 700mV^, a saturation occurs, but the EvaQuad shows no phase reversal, unlike the standard circuit. In the standard quad, Q1's collector waveform is in phase with the base voltage: this means that any feedback caused by a combination of input resistance and Ccb capacitance will be positive, increasing instabilities. In the Evaquad, Q5's collector has 0V AC potential, and this couldn't happen. Moreover, should Q6 be used as an input, voltages at out2 and tp1 will be antiphase, meaning that Q9's capacitance will play its normal role of Miller and contribute to stabilize the thing. Rule N°2: do not misunderestimate me too much either. ![]() The second pic compares the linearity of the two versions: the raw Xquad is superior, because the cancellation effects are more accurate.
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#216 |
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diyAudio Member
Join Date: Mar 2004
Location: Krakow
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![]() do you have the idea hot to prevent this circuit from the saturation? I attached a linearizion idea circuit which is a bit similar to Xquad, o found this somewhere on the net...
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regards, Pawel |
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#217 |
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diyAudio Member
Join Date: Nov 2007
Location: Dallas
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I never saw any saturation with the plain quad.
Then again, I have that active tail thing goin on... Keeps the quesscent roughly equal all times. . Raw xquad is working better in this instance than Evaquad or Evaquad wth driver collectors parrallel. I'm also driving an emitter drop to the rail, which isn't a huge voltage swing on the collector. Last edited by kenpeter; 1st September 2011 at 11:46 AM. |
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#218 |
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diyAudio Member
Join Date: Nov 2007
Location: Dallas
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Where is the problem, cause I'm just not seeing it.
No transistor of this quad loses collector voltage, even in moderate clipping, its all good... The two waves in the center (blue maybe little hard to see) are actually all four voltages of the xquad. The left and right closely overlap, both sides look as-if transistors bias like diodes. Differential currents vary, but differential voltages are held nearly equal. Its definitely doing something though, distortion is unmistakably reduced by presence of the xquad. No collectors here ever dip below the base voltage. I have no idea what is this "phase reversal" you say when the collector saturates. Do you simply mean the quad would stop reversing things working as a quad? Saturated behavior would revert to normal LTP ??? I don't think this tail allows the latched condition to exist. Even if you hit it with a transient huge enough to make one transistor saturate, and phase revert to uncrossed LTP. It would quickly be put back to right. Last edited by kenpeter; 1st September 2011 at 12:33 PM. |
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#219 | ||
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diyAudio Member
Join Date: Sep 2006
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Quote:
At least under normal working conditions. But to prevent a latch-up during some freak event, there has to be some form of safety net, it would be suicidal to leave the circuit do whatever it wants, that's the reason for the diode clipper at the input. But when a larger dynamic is required, as in the Tringlinator, a solution is to increase the Vbe of the lower transistors, by means of resistors or zeners f.e. If you look attentively at the schematic, you will see that that's what is done there. Incidently, it leaves more Vce space to breathe for the transistors. Quote:
It simply mimics the effect of a LTP, but with a diode to replace the other transistor. The compensating effect is already crude in a LTP, it is equivalent to assume that exp(-k*V)=-exp(k*V), but with two heavily dissimilar components, it will be worse. The only advantage that I can see in this circuit is the fact that the bias current is recycled, thus halving the current consumption compared to a LTP. But it costs two big e-lytics, and a similar trick could be used with transistors. Not of a great practical value.
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#220 | |||
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diyAudio Member
Join Date: Sep 2006
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That's in sim. With a real circuit, you have 99% chances the circuit locks up as soon as it is powered. I know, I've been there. In the sim try to put an .ic V(base of Q2)=2v, I think it will latch up. Quote:
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