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Vallon VMH3CS Mine Detector
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Originally posted by KingJL View PostWell, I've done three more... Hey, I am getting good at this! Increased the oven time to 30 min @ 250 deg F (121 deg C), freezer time to 30 min.
[ATTACH]36840[/ATTACH]
The modules are not wired up yet but all in the box plus Li-ion batteries to check fit. The data cable is the one in the top strain relief gland.
There is an Australian company that specialises in curly cables. It is worth looking at their website. http://www.premiumproductions.com/curlycords/
Eric.
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PeliPulse
Here is the latest incarnation of the Vallon VMH3CS.
It all fitted neatly into the 1050 Pelican case with the Li-ion batteries. The top of the case has the single control switch; the cable to the LED indicator and push button panel, and headphone output. The bottom end of the case has the connector for the search coil or probe.
The case is mounted on a 2 inch wide waist belt threaded through a stainless steel clip on the back of the box. In use, the best position seemed to be with the box just round the back at waist level. This keeps the one control, which is basically the on/off switch, within easy reach, and is the most comfortable when bending forward or digging.
The 8 conductor cable goes around the back to the chest mounted box which houses the push button control panel and LED signal indicator. Also in the box is a piezo speaker which is easily heard, as long as the surf is not crashing too loudly, but with a waterproof volume control that can adjust the sound almost to zero. If the conditions or preference is for headphones, then these can be plugged into the connector on the top of the box, which then disables the speaker in the chest unit. The chest unit mounted very conveniently on the chest harness for a Hero camera. The chest box disconnects from the cable by means of the mini DIN connectors for which I have made a sleeve which is watertight when mated. The box also slides off the harness mount.
The push buttons on the chest box control sensitivity, audio volume, pinpoint mode, and ground balance if needed. Battery state is also shown on the LED bargraph when switching on.
The concept is that one can search in water to waist height with the main box being submerged at times. The chest mounted control and indicator is mainly out of the water but will survive the inevitable wave splash. In fact it is only the 1/4 hole for the piezo speaker which limits the submersibility as I have made sure that the small Vallon housing that contains the push switches is completely sealed.
Field/water testing has yet to be done but the concept appears good so far, with the unit being easy and non tiring to use.
Eric.
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Originally posted by Qiaozhi View PostEric - It has just dawned on me that you have the Vallon completely in pieces! Does that mean you've been able to probe the circuit and discover how this detector can detect such low conductivity targets while using a 1.5mH coil?
The main electronics is in the grey box and consists of two SM boards of equal size piggy backed together. Both sides of the boards are loaded with components and can't be unplugged from each other. They are probably multilayer boards from the component density and would be a nightmare to unravel the details. It is all programmed in firmware too. All I have gleaned from a quick look at the boards is that the bipolar TX is probably an H bridge arrangement as there are four Mosfets close together. Where the RX preamp is, I do not know. Everything is covered in a coating of laquer so that even probing for voltages or waveforms involves penetrating this layer.
I do not have any faulty modules, otherwise I might probe deeper, but I am happy at the moment just shifting the black boxes around to make a detector that is easy to use on land and in water.
One thing I have learned is that it is easy today to power things off 3.7V Li-ion batteries. I have just received an up converter the size of a postage stamp where you can put any voltage above 2V in and get an adjustable voltage out of whatever you want up to 20V. I have it running a detector right now that requires 15V and it seems to work a treat. Prior to that I was using 10AA batteries!
Eric.
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Originally posted by Qiaozhi View Post... how this detector can detect such low conductivity targets while using a 1.5mH coil?
The magnetic field is proportional to the ampere-turns. Inductance is proportional to the square of the no. of turns. Given two coils (300uA and 1500uA) with the same diameter, the 1500uH coil at 0.44 amperes creates the same field as the 300uH coil at 1 ampere. ( sqrt(300) x 1A = sqrt(1500) x 0.44A )
The smaller current in the 1500uH compensates for the larger time constant and the transients of both coils reach the sampling state mor or less with the same delay. To compensate further, the receive singnal in the 1500uH is 5x stronger.
So I think it's perfectly possible to measure low conductivity targets due to the lower current taking less time to decay and the higher sensitivity allowing measurements with a slightly longer delay.
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One thing I have learned is that it is easy today to power things off 3.7V Li-ion batteries. I have just received an up converter the size of a postage stamp where you can put any voltage above 2V in and get an adjustable voltage out of whatever you want up to 20V. I have it running a detector right now that requires 15V and it seems to work a treat. Prior to that I was using 10AA batteries!
Eric.
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Originally posted by Teleno View PostFor lack of any schematic I'll venture a guess.
The magnetic field is proportional to the ampere-turns. Inductance is proportional to the square of the no. of turns. Given two coils (300uA and 1500uA) with the same diameter, the 1500uH coil at 0.44 amperes creates the same field as the 300uH coil at 1 ampere. ( sqrt(300) x 1A = sqrt(1500) x 0.44A )
The smaller current in the 1500uH compensates for the larger time constant and the transients of both coils reach the sampling state mor or less with the same delay. To compensate further, the receive singnal in the 1500uH is 5x stronger.
So I think it's perfectly possible to measure low conductivity targets due to the lower current taking less time to decay and the higher sensitivity allowing measurements with a slightly longer delay.
Is the signal amplitude not proportional to the turns of the coil? not the inductance.
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For up-converters, it's worth looking at hobbyist modules like those made by Pololu and others. (I have plans for one of these 5 Volt output modules to reduce battery pack size)
Example:
http://www.hobbytronics.co.uk/batteries
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Originally posted by Ferric Toes View PostAll I have gleaned from a quick look at the boards is that the bipolar TX is probably an H bridge arrangement as there are four Mosfets close together.
In which case, an H-bridge arrangement would be using the shield as the live connection on one polarity. Therefore I was wondering if the coil itself is actually two loops in anti-phase (probably bipolar wound). But ... if that was true, then your homemade coil would produce a unipolar, rather than a bipolar pulse.
There's a puzzle here to be solved .....
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Originally posted by Qiaozhi View PostI suspect that's not the case, as earlier you stated that the coil is single stranded with an outer mesh shielding, and the connector is 7-pin with the centre pin as live. All other six connectors are wired together to form an outer shield, and connected to the coax braid. In which case, an H-bridge arrangement would be using the shield as the live connection on one polarity. Therefore I was wondering if the coil itself is actually two loops in anti-phase (probably bipolar wound). But ... if that was true, then your homemade coil would produce a unipolar, rather than a bipolar pulse. There's a puzzle here to be solved .....
The parameters described by Eric:
Measured voltage at the coil = 6Volt,
Measured current: 1amp at 10usec... near constant for the next 40 usec,
250V flyback, transmit pulses 530 usec apart alternating
The only thing that i don't remember him stating was a HV kickstart pulse the same polarity of the main TX pulse, but I can see no way to get that 1 amp coil current within 10 usec without it.
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Originally posted by Skippy View PostFor up-converters, it's worth looking at hobbyist modules like those made by Pololu and others. (I have plans for one of these 5 Volt output modules to reduce battery pack size)
Example:
http://www.hobbytronics.co.uk/batteries
I have machined a small housing for the board, which I will wrap in copper shielding tape and ground to the electronics in the detector (my viscosity meter) as there is bound to be a bit of radiation from the inductor. I didn't notice any effect on the first test though.
Eric.
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Originally posted by KingJL View PostI have tried to model the TX based on Eric's descriptions/observations at the beginning of this thread. The model indeed requires 4 mosfets, but not as an H-Bridge.
The parameters described by Eric:
Measured voltage at the coil = 6Volt,
Measured current: 1amp at 10usec... near constant for the next 40 usec,
250V flyback, transmit pulses 530 usec apart alternating
[ATTACH]36934[/ATTACH]
The only thing that i don't remember him stating was a HV kickstart pulse the same polarity of the main TX pulse, but I can see no way to get that 1 amp coil current within 10 usec without it.
Would you mind posting the LTSpice files?
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Originally posted by Qiaozhi View PostI suspect that's not the case, as earlier you stated that the coil is single stranded with an outer mesh shielding, and the connector is 7-pin with the centre pin as live. All other six connectors are wired together to form an outer shield, and connected to the coax braid.
In which case, an H-bridge arrangement would be using the shield as the live connection on one polarity. Therefore I was wondering if the coil itself is actually two loops in anti-phase (probably bipolar wound). But ... if that was true, then your homemade coil would produce a unipolar, rather than a bipolar pulse.
There's a puzzle here to be solved .....
Eric.
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