Originally posted by KingJL
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Originally posted by KingJL View PostTX current waveform (triangular, half sine, trapezoidal, etc.).
As food for thought about the above discussion, I give you a link to an article to tickle your brain cells.
http://iieta.org/sites/default/files..._A/54.2_02.pdf
Now that is is a great little read... thanks for sharing.
Cheers
Mdtoday
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Originally posted by Ferric Toes View PostHave a read of this article. It changed my thinking on using expensive Litz wire.
https://engineering.dartmouth.edu/in...s/stranded.pdf
Eric.
Very good read with practical applications, thanks for sharing Eric.
Cheers
Mdtoday
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Originally posted by KingJL View PostTX current waveform (triangular, half sine, trapezoidal, etc.).
What you are doing is commendable and worthy of continued efforts. However, I would also think of your frame of reference... "minimum sample delay". In reference to what? In reference to removal of TX input pulse, actual MOSFET current shut-off (can be in excess of 2 usec after removal of gate signal), after coil current achieves some threshold level, etc. What is the objective? To achieve a fast coil or to detect a specific minimum TC target goal? To achieve the later does not necessitate the former... it is one means to achieve the result, but is not the only one. In fact I know of one detector that has excellent performance against a 3-5 usec TC target and samples at 50 usec after TX turn-off with a sample width of 50 usec... it really does not care about "how fast" the coil is (it has a TON of capacitance in the TX). What really needs to be thought about during observations of target responses is what is actually happening with target eddy currents within the context of the exciting TX current waveform (like Carl keeps saying "coil current waveform, not voltage"). Then you can implement a suitable solution to obtain the desired result. But that is probably suitable for a separate thread and discussion.
As food for thought about the above discussion, I give you a link to an article to tickle your brain cells.
http://iieta.org/sites/default/files..._A/54.2_02.pdf
would like to chart AWG28 solid that I have been using to make my coils to see if it charts a TC just over .3usec projected on the chart. At 5TC's, 1.5usec AWG28 would lose 99% of it's peak signal .http://www.geotech1.com/forums/attac...4&d=1526683069
Interesting about detecting a 3usec TC target with a 50usec delay. I'll have to try and understand how it does it.
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Originally posted by green View PostInteresting about detecting a 3usec TC target with a 50usec delay. I'll have to try and understand how it does it.
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Originally posted by KingJL View PostThe reason is the TX/coil current waveform... The detector is the Fisher Impulse which I believe was designed by Dave Johnson (Dave J). That is the problem I have with referencing sample time relative to TX-off. In my opinion, sampling needs to be referenced to the trailing boundary of the coil current waveform envelope. If you reference the sample timing to the trailing boundary of the coil current waveform enveope, the sample time for the Impulse becomes ~15 usec.
The impulse is a bipolar TX. By referencing the sample period to the trailing edge of the coil current envelope, the sample delay is < 15 usec (closer to 5).Attached Files
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Thanks Kingjl, is it this circuit ? always been curious about it, DaveJ has said a few times its worth investigating.Attached Files
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The focus on the impulse is probably dragging Green's thread a little off track. The reason I introduced it was to emphasize two points. (1) "minimum sample delay" to what reference, and (2) a fast coil circuit is not the only way to achieve detection of small resistive targets... there are other methods. I think the discussion of small fast tau target detection and the focus on the religeous need for ultra fast coils actually deserves it's own thread. There are a lot of moving parts to the physics that need to viewed and understood as an integral and not in isolation. There is no "holy grail"!!
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Have a read of this article. It changed my thinking on using expensive Litz wire.
https://engineering.dartmouth.edu/in...s/stranded.pdf
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Originally posted by KingJL View PostThe focus on the impulse is probably dragging Green's thread a little off track. The reason I introduced it was to emphasize two points. (1) "minimum sample delay" to what reference, and (2) a fast coil circuit is not the only way to achieve detection of small resistive targets... there are other methods. I think the discussion of small fast tau target detection and the focus on the religeous need for ultra fast coils actually deserves it's own thread. There are a lot of moving parts to the physics that need to viewed and understood as an integral and not in isolation. There is no "holy grail"!!
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Originally posted by green View Post... I've always referenced to coil off command thinking that made the most sense, maybe not. If there is a better way, I'm all for it.
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Originally posted by KingJL View PostI have wrestled with the refernce point for well on to 2 years now. For it to have any meaning, "sample time" must have the same reference from circuit to circuit. Personally, I have come to using the point to where coil current has decreased to 1 mA, for my personal comparisons. That way, it takes into account the actual removal of excitation of the target and takes away some of the mystery of why one particular detector appears so sensitive to fast tau targets and another is not.
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