Originally posted by simonbaker
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DEEPER PI DETECTION DEPTH
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Originally posted by Qiaozhi View PostI don't think Midas is disputing that the LTSpice inductor model is behaving the same as an identical discrete model. His comment is referring to the fact that the parallel capacitor in the LTSpice inductor model has zero ESR. In other words there's no way to define an equivalent series resistance for the parallel cap. Hence the glitches. If you build the same network with discrete parts, you can then include the missing ESR. The best option would be to use a parameterized subcircuit for an air coil in place of the inductor model.
On the other hand, does a real coil's parasitic capacitance have an ESR? What physically would cause that? Wouldn't the electric field just jump across the windings with almost no resistance? Or are we talking about a tiny-tiny but significant amount of resistance?
Who knows, maybe those 60A glitches in your sim exist in real life, but our measuring equipment can't pick them up, and they too transient to matter?
-SB
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Originally posted by simonbaker View PostHow do you capitalize on that wide-band information? If you don't use it wisely, you are better off using narrow band techniques because you are picking up a lot more noise with wide-band, it would seem.
-SB
that's a good question.Any ideas?
I for one would take all possible spectral energy of the response. And not all spectral bands do have the same noise level.
BTW, the VLF principle is taking an huge advantage of the narrow band (high gain at resonance and high suppression on the other frequency sides). And it's so efficient.
Despite of the fact, that a PI detector performs a wide band principle, it throws away a lot of the spectral response however. All the super high dI/dt (100 kA/s .. 1 million A/s) is mostly wasted.
Aziz
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Originally posted by simonbaker View PostLet's get a full simulation including the output of the preamp that agrees with the Carl's real tests showing 15% more output for the flat top charging pulse. I'd like to see what accounts for that extra 15%.
Up for it, Tinkerer?
-SB
Not to forget that the coil arrangement should be induction balanced.
Then we could really compare the real circuit with the simulated circuit and fine tune them both.
Let's do it!!!!!
Tinkerer
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Originally posted by Tinkerer View PostIt would be a good start if we could get a simulation of the target response and get this response into a RX coil and from the RX coil into the preamp.
Not to forget that the coil arrangement should be induction balanced.
Then we could really compare the real circuit with the simulated circuit and fine tune them both.
Let's do it!!!!!
Tinkerer
If not, basically just need to slap in the RX coil, add some parasitic components, add the preamp circuitry, to your existing sim. Delete the unused target coupling coefficients (or delete the unused targets completely).
Then start tweaking the coupling coefficients of the TX coil to RX coil and target to RX coil.
Of course good target models are desirable, but start with what we have.
-SB
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Originally posted by simonbaker View PostOk, my slowness, I didn't get that, thanks. Yes, it seems we may have a circuit where we need a more sophisticated model for an inductor than the LTSpice model. Of course you can keep going, dividing the coil into more and more elements, have to stop somewhere...
On the other hand, does a real coil's parasitic capacitance have an ESR? What physically would cause that? Wouldn't the electric field just jump across the windings with almost no resistance? Or are we talking about a tiny-tiny but significant amount of resistance?
Who knows, maybe those 60A glitches in your sim exist in real life, but our measuring equipment can't pick them up, and they too transient to matter?
-SB
Yes its probably not a large ESR but there's an infinite gulf between very small and zero. You can tell how unrealistic it is because its basically impossible to switch the mosfet in this model without getting massive drain-gate shoot through.
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Originally posted by Midas View PostPretty much every real component has resistance (except for those damn superconductors...) and having no capacity to enter the ESR of the parasitic capacitance makes the inductor model useless in any switched inductor application, and probably introduces significant inaccuracies in EVERY application. Sure we can work around and make a discreet model but we shouldn't have to.
Yes its probably not a large ESR but there's an infinite gulf between very small and zero. You can tell how unrealistic it is because its basically impossible to switch the mosfet in this model without getting massive drain-gate shoot through.
-SB
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Originally posted by simonbaker View PostSince LTSpice was developed primarily to analyze switching power supplies, it would be surprising that the inductor model would be so inadequate. Maybe this case should be posted on the LTSpice group to see if this is a known problem or if they can shed light on our simulation. Is it possible that: huge spikes exist in real life but are absorbed in other ways; or the spikes we see are not the fault of the inductor model but the other components around it (like ideal wires, mosfet model, etc.)?
-SB
With those thoughts in mind I made the following discrete model. Its hard to get your head around how much resistance there should be between all the connect points for a 15 ohm coil but its a start. It still has some weird current spike during switch on but the switch off is a lot better. Also removing the damping resistor doesn't result in the kind of oscillations I would expect so its obviously still not perfect.
Edit: Yeah actually.. its electrically identical to one of Simons earlier post. Lol I think we can burn this extra wheel.. never mind its been fun.
The question over what proportion of the total resistance is taken by each component remains though. It may not be 50/50.Attached Files
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The Dark Pulse Theory
Hi guys,
the Dark Pulse Theoryâ„¢ (nice name - isn't it?
) states, that there is no free lunch for you! I'm so sorry for this bad news. But it is very overdue now.
The EM pulse has a spectral energy, which is "seen" by the inductively coupled target and is responding to this pulse accordingly. The TX -> Target -> RX system has a frequency response as well (well, we can see it as a multi-stage filter response).
The nature offers you the maximum possible available information by physics law. All you can do is making either worse or loosing/throwing away that amount of available information.
You can easily see the proof of this statement by making a simple AC analysis (frequency response analysis) for different time constant (TC) targets. I have made this for four different TC targets for you. For your convenience, I'll put the spice file and you can play with it.
Now looking forward to the interesting discussion.
Cheers,
The Dark Aziz
Attached Files
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Originally posted by Midas View PostPretty much every real component has resistance (except for those damn superconductors...) and having no capacity to enter the ESR of the parasitic capacitance makes the inductor model useless in any switched inductor application, and probably introduces significant inaccuracies in EVERY application. Sure we can work around and make a discreet model but we shouldn't have to.
Yes its probably not a large ESR but there's an infinite gulf between very small and zero. You can tell how unrealistic it is because its basically impossible to switch the mosfet in this model without getting massive drain-gate shoot through.
Of course, I still have a lot to learn about simulations, but most of the time when there are differences, I can find the cause in my own mistakes.
Tinkerer
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Originally posted by Midas View PostIndeed, I wouldn't have expected it to be so fundamentally flawed either. Thinking about it a bit more the neglected resistance isn't so small either, since the parasitic capacitance is coupling to the mosfet drain through the coil it has go through at least some of the coils resistance. Also there should be resistance between the coil and its parasitic capacitance, otherwise the coil could potentially oscillate forever, which of course isn't possible.
With those thoughts in mind I made the following discrete model. Its hard to get your head around how much resistance there should be between all the connect points for a 15 ohm coil but its a start. It still has some weird current spike during switch on but the switch off is a lot better. Also removing the damping resistor doesn't result in the kind of oscillations I would expect so its obviously still not perfect.
Edit: Yeah actually.. its electrically identical to one of Simons earlier post. Lol I think we can burn this extra wheel.. never mind its been fun.
The question over what proportion of the total resistance is taken by each component remains though. It may not be 50/50.
General thoughts:
It may be true that our PI coils with their unique flyback pulse are a special case where the LTSpice inductor model is too simple. In switching power supplies, I guess there are usually some hefty capacitors nearby that would mask the lack of ESR in the coil parasitic capacitor.
However, we have to be careful about making conclusions based on tweaking models. Although tweaking some ESR into the inductor model may make our simulation look better, it doesn't prove we are tweaking the right component. Maybe the inductor is working quite close to a real one, but our MOSFET model is too simple and we see an effect that we wrongly blame on the inductor. Or perhaps we need to put a little inductance and resistance into our circuit wires.
I see your model with what looks like 30 ohms of ESR in the parasitic capacitance. That may fix the simulation, but it just doesn't seem realistic to me. However, I really don't know. I guess my physical interpretation of the parasitic capacitance would be a current that jumps directly across from winding to winding through the insulation and does not really travel down the wire like the inductor current. It is plausible to me that the capacitive current could have extremly low ESR.
But I just don't know. It would be great if we could actually set up a test rig to measure these parameters directly, but given the tiny parameters, how would we do that? Even oscilloscope probes would probably be a big factor.
In any case, we may in fact need a more realistic model for the inductor for PI simulations, and it would be good to have one. Your model looks like a good start, and I believe there is a way to package it as a component we can easily use in LTSpice -- I hope.
I still wonder if there is some virtually pure capacitance in parallel with the coil that should be modeled also. Hard to know when to stop with a lumped approximation of a distributed real-life component.
Regards,
-SBAttached Files
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Originally posted by Aziz View PostHi guys,
the Dark Pulse Theoryâ„¢ (nice name - isn't it?
) states, that there is no free lunch for you! I'm so sorry for this bad news. But it is very overdue now.
The EM pulse has a spectral energy, which is "seen" by the inductively coupled target and is responding to this pulse accordingly. The TX -> Target -> RX system has a frequency response as well (well, we can see it as a multi-stage filter response).
The nature offers you the maximum possible available information by physics law. All you can do is making either worse or loosing/throwing away that amount of available information.
You can easily see the proof of this statement by making a simple AC analysis (frequency response analysis) for different time constant (TC) targets. I have made this for four different TC targets for you. For your convenience, I'll put the spice file and you can play with it.
Now looking forward to the interesting discussion.
Cheers,
The Dark Aziz
We are ringing a bell and trying to figure out what kind of bell it is. We don't expect the sound of the bell to be anything like the hammer blow we hit it with. But it will hopefully tell us all about the bell.
Cheers,
-SB
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Originally posted by simonbaker View PostDon't forget Aziz, the information in the TX pulse is not what we are trying to recover. We're really trying to estimate the system parameters defining a target. The reponse has that information even though the bandwidth is radically different from the TX pulse.
We are ringing a bell and trying to figure out what kind of bell it is. We don't expect the sound of the bell to be anything like the hammer blow we hit it with. But it will hopefully tell us all about the bell.
Cheers,
-SB
the simple but fundamental AC analysis tells a lot. You should think about it.
BTW, you all should do more AC analysis rather than transient analysis.
Cheers,
Aziz
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Originally posted by Aziz View PostHi SB,
the simple but fundamental AC analysis tells a lot. You should think about it.
BTW, you all should do more AC analysis rather than transient analysis.
Cheers,
Aziz
-SB
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Originally posted by Tinkerer View PostThe Drain-Gate shoot through with real mosfets, when using high A coil currents, is exactly the problem that I have. To me, used to real circuits, the simulations look quite good.
Of course, I still have a lot to learn about simulations, but most of the time when there are differences, I can find the cause in my own mistakes.
Tinkerer
Anyway I'm starting to realize the danger of simulations... you can spend hours tweaking them never really learning anything with confidence.
Originally posted by simonbaker View PostHowever, we have to be careful about making conclusions based on tweaking models. Although tweaking some ESR into the inductor model may make our simulation look better, it doesn't prove we are tweaking the right component. Maybe the inductor is working quite close to a real one, but our MOSFET model is too simple and we see an effect that we wrongly blame on the inductor. Or perhaps we need to put a little inductance and resistance into our circuit wires.Attached Files
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