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Interesting about the tau from 1.6 to 37us. How does the signal amplitude increase from 1x to 32x? This test target gives indeed valuable information. I will have to make one.
For gold nuggets:
If anyone wants to further the cause, I accept donations of gold nuggets in any size and variation. Any quantity.
Tinkerer
I'm also willing to 'take one for the team' however I'm not as generous as you Tinkerer, I have a 5 nugget limit per person per day, and please don't send me nuggets any bigger than 250kg. I don't have any mechanical lifting equipment and the courier got really annoyed the last time that happened.
Thats a fair point. Even face on a laminated target thick enough for the skin depth to come into play would have reduced losses over an identical solid target. You could call it a 'litz target'. Anway of course this is entirely academic and certainly doesn't invalidates their use in the manner that Carl suggests.
Thats a fair point. Even face on a laminated target thick enough for the skin depth to come into play would have reduced losses over an identical solid target. You could call it a 'litz target'. Anway of course this is entirely academic and certainly doesn't invalidates their use in the manner that Carl suggests.
I have cut a batch of alu foil targets.
1/2"x1/2" is the smallest that I can detect with the 1meter coil, inside the house.
Then I have 1"x1/2", 2"x1/2", 1"x1", 1"x1"x2, 1"x1"x4, 1"x1"x8 layers.
I am working on it, but time is sparse at the moment so please be patient.
In the meantime it would be nice if somebody would give it a try too, so we could compare results.
I have a 3"x3" aluminum foil and a 3"x3" gold leaf that I commonly use.
The 1/2"x 1/2" is only detected at the center of the coil at 0 level with the 1 meter coil, but I think it will work as the minimum target for that coil and my present preamp breadboard, taking the output of the integrator. Also my TX is at 50% power, just making a quick and dirty trial to decide on a setup to do the series of tests.
no I don't say do the FFT on the response signal. I'm just saying look at the AC response in the posting ( http://www.geotech1.com/forums/showp...&postcount=221 ).
I'm just saying to do more AC response spice simulations. It answers some fundamental (but interesting) questions.
So, what's the simple graph is telling us?
Put the following command line somewhere and change the transmitter inductance (don't remove the L=300µ command):
.step param L list 150µ 300µ 600µ
And look what happens.
Report all here, what you have found.
Cheers,
Aziz
Exactly!
I'm new to this MD stuff, but I have some experience with spice. It dawned to me unfortunately completely independent from this discussion, as it could spare me a lot of time and effort. I played with a Tx of 3900's circuit and to do so I modeled a "coin", yet with values scaled up - works the same. Took me some time to come up with it
Anyway, Rx loop is a LP filter. When its time constant - or better say impedance match is achieved, you'll not lose much in amplitude, but the phase curves become steeper. The peak voltage is much lower (lower high frequency content), but the zero crossings become sensible. I mean REALLY sensible.
To cut the crap short - it is a no-go for high impedance amplifiers.
High series resistance gets coupled with target resistance, and when it is high it completely obliterates phase information. They both act as HP so High Tx series resistance is a bad thing.
With all these filters in a system, a short pulse is a bad thing because it is actually made of two events: rise and fall. Both of them are propagated in time domain and screwing up detection. And it comes with high voltage spikes.
Stepped voltage at Tx produces single events which are more sensible and have neat zero crossing. Because there are no overlapping events it will be a better choice for discrimination.
So, with all due respect to all, good detection/discrimination may begin when phase response is taken care of - both in PI and IB. Tau of various targets is the same for both of them.
Exactly!
I'm new to this MD stuff, but I have some experience with spice. It dawned to me unfortunately completely independent from this discussion, as it could spare me a lot of time and effort. I played with a Tx of 3900's circuit and to do so I modeled a "coin", yet with values scaled up - works the same. Took me some time to come up with it
Anyway, Rx loop is a LP filter. When its time constant - or better say impedance match is achieved, you'll not lose much in amplitude, but the phase curves become steeper. The peak voltage is much lower (lower high frequency content), but the zero crossings become sensible. I mean REALLY sensible.
To cut the crap short - it is a no-go for high impedance amplifiers.
High series resistance gets coupled with target resistance, and when it is high it completely obliterates phase information. They both act as HP so High Tx series resistance is a bad thing.
With all these filters in a system, a short pulse is a bad thing because it is actually made of two events: rise and fall. Both of them are propagated in time domain and screwing up detection. And it comes with high voltage spikes.
Stepped voltage at Tx produces single events which are more sensible and have neat zero crossing. Because there are no overlapping events it will be a better choice for discrimination.
So, with all due respect to all, good detection/discrimination may begin when phase response is taken care of - both in PI and IB. Tau of various targets is the same for both of them.
I can't quite understand what you are saying.
Can you explain using some formulas/numbers or show your Spice simulations that demonstrate what you are trying to say?
Yeah, it is a bit frustrating not to see it as an animated powerpoint presentation .
Aziz put a nice LTSpice model with a quoted post, where all the components had regular values. By first glance you'll see nothing much going on, but there is. You may easily play with values and see how the whole shebang gets affected. Everything is in AC (mag/phase) domain.
Now, with receiver signal having a 0 DC, it is obvious that whatever happens in time domain right after a PI pulse, must go through zero, and a whole signal integrated from pulse to pulse is zero. If target's tau is not affected by Tx coil's resistance (you may observe it as a transformer), you'll get a Rx signal that passes through zero with the same delay from PI pulse, regardless of depth/size, hence discrimination.
Attached is a LTSpice simulation of a White's oscillator working as a PI exciter, and a step voltage excitation I was meditating upon. There are ".step param" options to play with, but these should work as they are. Please note how clean the signal gets with stepped exciter.
Aziz, I like what you do, and it is in many ways fundamental. But if you really wish to drive attention, and also keep people on the same track, you could provide some hints as well
Aziz, I like what you do, and it is in many ways fundamental. But if you really wish to drive attention, and also keep people on the same track, you could provide some hints as well
Thank you
-You all are driving me mad! -
Where is the mental doctor for me?
You shouldn't try to guess, what I'm thinking. The question is plain straight forward.
What can you extract basic fundamentals on the mentioned AC response?
It says to me that with the same coupling, amplitude (target size and/or distance) remains the same ... within reasonable frequency range. In case I'm terribly wrong, could you please provide some hints?
Again, don't look at the phase response yet. Don't look at the discrimination ability. Forget the discrimination at all.
We want to focus to the fundamentals only.
Go ahead guys.
Cheers,
Aziz
Aziz,
Like everyone else I'm perplexed about exactly what the question is your asking but to keep the ball rolling I'll attempt to draw some (though quite probably not the ones your driving at) conclusions from your plot.
* Long time constant targets seem to respond maximally to a broader range of frequencies.
* With shorter time constants the maximum target response occurs at a higher frequency.
* As the frequency increases into the Mhz range target time constants starts to become irrelevant and all the target responses diminish together.
Yeah, it is a bit frustrating not to see it as an animated powerpoint presentation .
Aziz put a nice LTSpice model with a quoted post, where all the components had regular values. By first glance you'll see nothing much going on, but there is. You may easily play with values and see how the whole shebang gets affected. Everything is in AC (mag/phase) domain.
Now, with receiver signal having a 0 DC, it is obvious that whatever happens in time domain right after a PI pulse, must go through zero, and a whole signal integrated from pulse to pulse is zero. If target's tau is not affected by Tx coil's resistance (you may observe it as a transformer), you'll get a Rx signal that passes through zero with the same delay from PI pulse, regardless of depth/size, hence discrimination.
Attached is a LTSpice simulation of a White's oscillator working as a PI exciter, and a step voltage excitation I was meditating upon. There are ".step param" options to play with, but these should work as they are. Please note how clean the signal gets with stepped exciter.
It is just a thought ...
Ok -- I gather your point is to consider designs using zero-crossing events as a way to discriminate, sounds good. However, it seems these schemes are really looking at ways to estimate the "time constant" (TC or "tau") of a target (assuming a simple L/R model for a target).
In general, I still have not heard a good explanation of how estimating the "tau" of a target tells me whether to dig or not. Anyone have some more data on how to interpret a particular "tau" once we have it in our little hot hands?
In general, I still have not heard a good explanation of how estimating the "tau" of a target tells me whether to dig or not. Anyone have some more data on how to interpret a particular "tau" once we have it in our little hot hands?
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