Here's a PM I received today from allahyarzadeh
I thought it would be better to reply to these questions in the Tech Forum, as I'm sure others would like to put forward suggestions for this worthwhile endeavour:
Hi,
sorry to bother you with my questions,
you are well known for your knowledge in metal detectors and coils,
I'm currently designing a humanitarian de-mining system funded by NGOs and UN charter ,and to be distributed with the people still living in the mine fields,as you may know there are lots of people dying nowdays in these fields.
I've designed a PI which is simple and some how very slow. I use it to mines with very low metal objects in them,which are as small as 3mm,
first of all I have problem with my device stability,and then comes speed and then comes ground effect,my device detects the soil itself when it comes near it,I have to upgrade it before complete it's production and distribution among ordinary people.
I use a 2mH coil with size of 20cm x 16cm Ellipse shape with stranded 0.8mm copper wire,
I Use Bu808 BJT transistor as switch ,30v power voltage to be switched on coil, and I use no damping resistor ,instead one 330 ohm (pulse rated non inductive ressistor) and six back to back diodes(1n4148 after them one 1k ohm resistor to ground and then it is my amplifier,one nasty old LM709 amplifier and then some S&H and other amplifiers until it reaches to ADC( a 18bit) .
in this configuration my 330 ohm resistor became very hot and the device need about 15 minutes to be completly stable,which is not good.
in analog amplification I have about 110db gain from main signal to detect small changes.
I use so many Technics to achieve more depth with increasing the back EMF peak voltage as high as 1000 volts and also in digital parts sampling from many areas and many pulses and then using some statistical Technics to omit noise and take out the real signal which has made my device too slow.
in this topology I had many high current consumption due to very high peak voltage and strong field.so I couldn't increase the frequency more than 100Hz.
Until I introduced with this forum and Guru's Post here I tried to use some mosfets with cascode we had a discussion here:
http://www.geotech1.com/forums/showt...879#post208879
http://www.geotech1.com/forums/showt...879#post208879
and I tried to use much less inductance for my coil and using a damping resistor ,using differential reading of signal ,
but this new one is really fast in responce but it's depth is not more than my previous design and stability is not ok again.
I wanted you to help me in this and answer some of my questions please ,
I know you are busy any of them you could answer please.
1- does more peak voltage guarantee me more depth?
2- what is optimal inductance of coil? I'm aware of low time constant of small gold nuggets,but I'm not going to find gold.I'm going to find small pieces of steel or ferrus metal, cr6 or sth.
3- how I should calculate the damping ressistor needed for damping the coil?what are the equations?
4- can I use blocking Fets instead of resistor and diodes,because I have many noise from there,
5- how I can achieve more than 120db gain for the main signal?(counting 24bit adc)
6- how I can undermine the ground effect which my device sees the earth as metal object when I near the coil to ground?
7- what frequency should I use? my previos device used 100 Hz which was very low for midpass filter and my 2nd circuit was 500hz ,what's the relation between frequency and coil and other specifications?
8- How I should build my coil? double d? monocoil? it is very better for me to recognise both right and left signal with double coils because before hitting the mines head with coil it could detect it.(it's some how vital)
9- do I need to shield my coil?with what? aluminium foils?
10 - I ordered a high voltage battery of 48v Li-ion battery with 5000mAh capacity,and I use this voltage to switch on my coil,to have more depth and more field, is it right?
11- I have a doubt about pulse signals I have one circuit with constant pulses and sample pulse, and in my second design I use to send some big pulses and some small pulses. What is the best timing and pulse?
----------------------------------------------------------------
My reply:
In summary;
You want to be able to detect targets as small as 3mm diameter. The target material will be small pieces of steel or ferrous metal, such as cr6 or sth. I assume cr6 refers to chromium plating, but what is sth?
There are problems with the current design involving slow response speed and ground effect (detects the soil).
The coil (20cm x 16cm) has 2mH inductance, and is wound with 0.8mm diameter stranded wire.
The TX coil transistor is a BJT, 30V supply voltage, and no damping resistor!
Flyback voltage reaches 1000V, and the pulse rate is 100pps.
Firstly, what is the decay constant for a 3mm diameter ferrous target?
Using the equation:
Where the conductivity of iron (Fe) is:
Hence:
= 2.95us
Therefore the eddy currents in the target will have completely decayed away after 5 * 2.95us = 14.75us
It has been recommended in some papers that you should aim for a main sample delay of one-tenth of the target object. In this case it appears we would ideally require a main sample delay of ~1.5us, which is extremely aggressive. Clearly this is not achievable with a 2mH coil inductance, a large coil current, and a low TX pulse rate of 100pps. I find it difficult to understand how it is possible to detect such a small target with the current setup. Unless it has something to do with not having a damping resistor. In which case, the RX waveform will be a decaying sinewave, and the detector is not really a PI after all, but more like some early Tandy and Heathkit designs that utilized this approach. This would also explain the problems with ground effect, as it's basically a TR-type detector without a GB channel.
The best way to determine the damping resistor value is to use a damping resistor tool. This consists of a 10k trimmer in series with a 200R resistor, and both in parallel with a 2k resistor. This gives an adjustment range from 181R to 1k672.
Monitor the preamp output, and adjust the trimmer for critical damping or slight undamping. Measure the final value, and replace with a fixed resistor.
Regarding TX output power - please read the attached document: "Coil Voltage vs Depth - from Tec".
Also, you should be aware that such a small target does not require a huge coil current to become saturated, and extra depth is subject to the sixth power rule.
I suspect the "ground effect" you are experiencing is either due to coil-to-soil capacitance, or a simple TR effect due to the damping resistor being missing. Once you get the coil critically damped, you could add a second sample pulse to achieve ground balance, but this means you will lose some depth, and create a movable target hole in the response. It might be worth exploring an alternative technique put forward by Teleno (reading from post #69 onwards) -> http://www.geotech1.com/forums/showt...-transmit-time
Personally I think you should reduce the coil inductance considerably, to at least 300uH, increase the TX pulse rate to as high as possible (considering the limitations imposed by software processing overhead), concentrate on reducing noise in the RX channel, and decide on a suitable method for ground balance that does not reduce depth or miss targets. You will also need to shield the coil in order to use early sampling. Suggested reading -> http://www.geotech1.com/pages/metdet...s/FastCoil.pdf
Anyone who wants to chip in, please do so.
I thought it would be better to reply to these questions in the Tech Forum, as I'm sure others would like to put forward suggestions for this worthwhile endeavour:
Hi,
sorry to bother you with my questions,
you are well known for your knowledge in metal detectors and coils,
I'm currently designing a humanitarian de-mining system funded by NGOs and UN charter ,and to be distributed with the people still living in the mine fields,as you may know there are lots of people dying nowdays in these fields.
I've designed a PI which is simple and some how very slow. I use it to mines with very low metal objects in them,which are as small as 3mm,
first of all I have problem with my device stability,and then comes speed and then comes ground effect,my device detects the soil itself when it comes near it,I have to upgrade it before complete it's production and distribution among ordinary people.
I use a 2mH coil with size of 20cm x 16cm Ellipse shape with stranded 0.8mm copper wire,
I Use Bu808 BJT transistor as switch ,30v power voltage to be switched on coil, and I use no damping resistor ,instead one 330 ohm (pulse rated non inductive ressistor) and six back to back diodes(1n4148 after them one 1k ohm resistor to ground and then it is my amplifier,one nasty old LM709 amplifier and then some S&H and other amplifiers until it reaches to ADC( a 18bit) .
in this configuration my 330 ohm resistor became very hot and the device need about 15 minutes to be completly stable,which is not good.
in analog amplification I have about 110db gain from main signal to detect small changes.
I use so many Technics to achieve more depth with increasing the back EMF peak voltage as high as 1000 volts and also in digital parts sampling from many areas and many pulses and then using some statistical Technics to omit noise and take out the real signal which has made my device too slow.
in this topology I had many high current consumption due to very high peak voltage and strong field.so I couldn't increase the frequency more than 100Hz.
Until I introduced with this forum and Guru's Post here I tried to use some mosfets with cascode we had a discussion here:
http://www.geotech1.com/forums/showt...879#post208879
http://www.geotech1.com/forums/showt...879#post208879
and I tried to use much less inductance for my coil and using a damping resistor ,using differential reading of signal ,
but this new one is really fast in responce but it's depth is not more than my previous design and stability is not ok again.
I wanted you to help me in this and answer some of my questions please ,
I know you are busy any of them you could answer please.
1- does more peak voltage guarantee me more depth?
2- what is optimal inductance of coil? I'm aware of low time constant of small gold nuggets,but I'm not going to find gold.I'm going to find small pieces of steel or ferrus metal, cr6 or sth.
3- how I should calculate the damping ressistor needed for damping the coil?what are the equations?
4- can I use blocking Fets instead of resistor and diodes,because I have many noise from there,
5- how I can achieve more than 120db gain for the main signal?(counting 24bit adc)
6- how I can undermine the ground effect which my device sees the earth as metal object when I near the coil to ground?
7- what frequency should I use? my previos device used 100 Hz which was very low for midpass filter and my 2nd circuit was 500hz ,what's the relation between frequency and coil and other specifications?
8- How I should build my coil? double d? monocoil? it is very better for me to recognise both right and left signal with double coils because before hitting the mines head with coil it could detect it.(it's some how vital)
9- do I need to shield my coil?with what? aluminium foils?
10 - I ordered a high voltage battery of 48v Li-ion battery with 5000mAh capacity,and I use this voltage to switch on my coil,to have more depth and more field, is it right?
11- I have a doubt about pulse signals I have one circuit with constant pulses and sample pulse, and in my second design I use to send some big pulses and some small pulses. What is the best timing and pulse?
----------------------------------------------------------------
My reply:
In summary;
You want to be able to detect targets as small as 3mm diameter. The target material will be small pieces of steel or ferrous metal, such as cr6 or sth. I assume cr6 refers to chromium plating, but what is sth?
There are problems with the current design involving slow response speed and ground effect (detects the soil).
The coil (20cm x 16cm) has 2mH inductance, and is wound with 0.8mm diameter stranded wire.
The TX coil transistor is a BJT, 30V supply voltage, and no damping resistor!
Flyback voltage reaches 1000V, and the pulse rate is 100pps.
Firstly, what is the decay constant for a 3mm diameter ferrous target?
Using the equation:
Where the conductivity of iron (Fe) is:
Hence:
Therefore the eddy currents in the target will have completely decayed away after 5 * 2.95us = 14.75us
It has been recommended in some papers that you should aim for a main sample delay of one-tenth of the target object. In this case it appears we would ideally require a main sample delay of ~1.5us, which is extremely aggressive. Clearly this is not achievable with a 2mH coil inductance, a large coil current, and a low TX pulse rate of 100pps. I find it difficult to understand how it is possible to detect such a small target with the current setup. Unless it has something to do with not having a damping resistor. In which case, the RX waveform will be a decaying sinewave, and the detector is not really a PI after all, but more like some early Tandy and Heathkit designs that utilized this approach. This would also explain the problems with ground effect, as it's basically a TR-type detector without a GB channel.
The best way to determine the damping resistor value is to use a damping resistor tool. This consists of a 10k trimmer in series with a 200R resistor, and both in parallel with a 2k resistor. This gives an adjustment range from 181R to 1k672.
Monitor the preamp output, and adjust the trimmer for critical damping or slight undamping. Measure the final value, and replace with a fixed resistor.
Regarding TX output power - please read the attached document: "Coil Voltage vs Depth - from Tec".
Also, you should be aware that such a small target does not require a huge coil current to become saturated, and extra depth is subject to the sixth power rule.
I suspect the "ground effect" you are experiencing is either due to coil-to-soil capacitance, or a simple TR effect due to the damping resistor being missing. Once you get the coil critically damped, you could add a second sample pulse to achieve ground balance, but this means you will lose some depth, and create a movable target hole in the response. It might be worth exploring an alternative technique put forward by Teleno (reading from post #69 onwards) -> http://www.geotech1.com/forums/showt...-transmit-time
Personally I think you should reduce the coil inductance considerably, to at least 300uH, increase the TX pulse rate to as high as possible (considering the limitations imposed by software processing overhead), concentrate on reducing noise in the RX channel, and decide on a suitable method for ground balance that does not reduce depth or miss targets. You will also need to shield the coil in order to use early sampling. Suggested reading -> http://www.geotech1.com/pages/metdet...s/FastCoil.pdf
Anyone who wants to chip in, please do so.

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