Some tests with TRT and target-no target charting, fig8 Rx and mono. Added a 139usec decay line to charts to compare actual decay with. Differential amplifier with fig8 Rx(Tx surrounds Rx), inverted input amplifier with mono (Rx, Tx).
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Originally posted by green View PostSome tests with TRT and target-no target charting, fig8 Rx and mono. Added a 139usec decay line to charts to compare actual decay with. Differential amplifier with fig8 Rx(Tx surrounds Rx), inverted input amplifier with mono (Rx, Tx).Attached Files
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Shouldn't you be using a proper silver 25c coin, not a clad one? It seem that it would be a worthwhile comparison, anyway, having data for both. There's quite a pronounced difference in conductivity between the (copper) core and the (CuNi) cladding. It may show up what is a target characteristic, what is test-jig related.
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Originally posted by Skippy View PostShouldn't you be using a proper silver 25c coin, not a clad one? It seem that it would be a worthwhile comparison, anyway, having data for both. There's quite a pronounced difference in conductivity between the (copper) core and the (CuNi) cladding. It may show up what is a target characteristic, what is test-jig related.
4msec Tx crAttached Files
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Originally posted by green View PostAdded two lines to chart posted above through 100 and 200us. Got a time constant closer to yours. Before I had my TRT I did what you did plus. Two recordings, no target and target. Subtracted no target from target recording(cancels no target offset in the beginning that I couldn't zero out with a mono coil) and charted difference linear-log with Excel. I'll try the old way with the quarter hopefully today. Didn't get straight line decay until closer to 200us delay with my TRT, included chart. Do you have a way to subtract and chart two recordings, target and no target? Wonder if a 600us Tx with your tester(first sample at 200us) wouldn't give a time constant closer to the 137us I got.
10.4us for the nickel looks good, wonder why your other method gives a different answer.
The first plot is triggered from the start of the TX (red trace) to confirm the TX width.
The second plot is triggered from TX end, as have previous plots of this type.
In the first plot, even though the TX pulse was long enough to fully saturate the coin (late time at turn on), waiting until 200uS after turn off is necessary to observe the single invariant true TC. of over 134uS.
To compensate for any variations in the zero base line, the target is removed after each measurement and a button is pressed to auto-zero the final dc amplifier stage. Obviously this does not apply to the scope'd plots I am currently doing.
Eric.
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Originally posted by green View PostQuarters look the same up to 120usec. Silver quarter, slower decay after 150usec.
4msec Tx cr
Also, by the same method, I measured a 4.4gm gold nugget from the Victorian goldfields, Australia. The TC is 23.8uS.
Eric.
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Originally posted by Ferric Toes View PostI have a 1964 silver quarter which I am told is 90% silver and 10% copper. IACS measures 88%. It requires a TX width of 800uS to fully charge and at 200uS start point the TC is 165uS. Increasing to 400uS start point the TC is 183uS.
Also, by the same method, I measured a 4.4gm gold nugget from the Victorian goldfields, Australia. The TC is 23.8uS.
Eric.Attached Files
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Originally posted by green View PostThanks for the testing. Something to compare against. Thought we were getting similar results. Wasn't getting near 183us with my silver quarter. Have been using constant rate instead of constant current. Some tests with a silver quarter constant current and constant rate. With amplifier not over scaling(top chart)all decays about 150us TC after 180us delay. With coin closer amplifier over scales, TC increased to 157usec all traces after 350usec delay. Constant current, constant rate and Tx time didn't seem to have much effect on time constant after a certain delay time.
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I'm still on the learning curve with the Picoscope and tried some other features today. The y axis scaling feature was useful as this enables the part of the waveform of interest to be magnified and the cursors set more accurately. I have also shifted the y zero to the bottom line. Today's results for clad and silver quarters as as attached. I measured both with a TX width of 800uS and at 300uS start point. My workshop temperature is also 19 - 20C.
Eric.
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Originally posted by Ferric Toes View PostI'm still on the learning curve with the Picoscope and tried some other features today. The y axis scaling feature was useful as this enables the part of the waveform of interest to be magnified and the cursors set more accurately. I have also shifted the y zero to the bottom line. Today's results for clad and silver quarters as as attached. I measured both with a TX width of 800uS and at 300uS start point. My workshop temperature is also 19 - 20C.
Eric.
[ATTACH]45342[/ATTACH] [ATTACH]45343[/ATTACH]
Eric, how much difference is the time constant if you take the first amplitude value at 300, 325, 350us with the method reply#204?Attached Files
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Tried a couple things yesterday. Exercised the brain without much success.
First: tried to calculate tau with input from Eric's chart http://www.geotech1.com/forums/attac...1&d=1549399390. (Vo=119@300us, Vt=77@350usec)What is the formula for calculating tau? Found a formula that worked with trial and error.
Second: tried to see if I could prove not straight line decay in the beginning isn't caused by skin effect. https://www.powerstream.com/Wire_Size.htm gives a frequency for 100% skin depth for different size wires. After some calculations, not sure if skin effect could be the cause. Maybe someone could try with the wire charts included. Recorded each target two times to check for repeatability. Both recordings the same until lower amplitude where noise caused difference. Looks like my scope has some error. A step about 1.25 divisions below .4 volt line on all the recordings as an example. Started with copper wire for targets. Thinking different thickness copper plates maybe 45mm square for the next try. Any thoughts appreciated.Attached Files
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Originally posted by green View PostI'm on a learning curve also. Increased chart size to see better what is happening. Appears straight line decay after approximately two target time constants. Wondering why two target time constants, and if target related. Maybe some targets take more or less than two time constants? Noticed I wasn't getting the same decay with clad quarters. Charted two with the largest difference of four coins I tried along with a silver quarter. Charted coin close to coil and spaced for near full scale signal at beginning. Clad and silver coins same location. Clad and silver chart same the first 200usec.
Eric, how much difference is the time constant if you take the first amplitude value at 300, 325, 350us with the method reply#204?
The results for the clad quarter for TC are 127.7uS, 136.3uS, 140.1uS for the ascending order of start points. For the silver quarter the results are 160.0uS, 171.3uS, and 175.9uS.
Clad plots
Silver plots
Eric.
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Originally posted by Ferric Toes View PostHi Green, I have further optimised my measurements by expanding the portion of the waveform to be measured as far as possible, and setting the digital filtering to reduce noise as much as I can. I used a long 1mS TX time for all measurements, so that should not be an issue. My start points are 150, 250, and 350uS, These are not as you requested as I had already done them before I saw your last post. I did not go to later starts than 350uS as noise will cause errors. You can see a slight ripple in the tail after the measuring window of the 350uS plots. I tried to get as close as possible to the 37% of the start amplitude, which is considerably better than before, due to the improved scaling. I doubt there is anything more I can do to improve things on these targets.
The results for the clad quarter for TC are 127.7uS, 136.3uS, 140.1uS for the ascending order of start points. For the silver quarter the results are 160.0uS, 171.3uS, and 175.9uS.
Clad plots [ATTACH]45363[/ATTACH] [ATTACH]45364[/ATTACH] [ATTACH]45365[/ATTACH]
Silver plots [ATTACH]45366[/ATTACH] [ATTACH]45367[/ATTACH] [ATTACH]45368[/ATTACH]
Eric.
Your decay looks real smooth. Is the Pico scope smoothing the decay? Read your reply again, missed the digital filtering the first time?
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Green : maths for exponential decay:
V = voltage; V0 = starting voltage; t = time difference; TC = time-constant, Tau.
V = V0 e -(t / TC)
=> ln (V / V0) = -t / TC
and: ln (V0 / V) = t / TC
You do have some dodgy 'scope ADC issues, I had noticed them before. I've forgotten ... your scope data ends up in an Excel table ? You could try the simple filter I posted in post #93.
Your plots of the 19mm straight wire length and the loops of the same gauge wire appear to show the same initial drop, which I would expect. There doesn't seem to be any evidence of a 'pause' at 22usec rate for any time, before the dominant full loop decay starts.
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