Originally posted by green
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Let us assume that the target has a 5uS TC. We would need a TX pulse at least 5 times longer than the target TC or 25 uS. The full stimulation of that target would require a coil with a coil discharge TC of one fifth the target TC or 1 uS. That means that we need a coil of 300 uH that has a 300 ohms effective damping resistance value. This effective value includes the input resistor to the first op amp stage which clamps the input resistor in parallel with the damping resistor during the flyback pules down to about 0.6V. If you set the delay to 10 uS your maximum target signal will be 2 TCs or about 86.5 percent lower than the maximum target induced signal.
Knowing the target TC can help you reverse engineer a coil resistance, inductance, effective damping value along with the proper TX and RX parameters for that target. Since target TCs are unknown, we tend to cluster our coil sizes/types and PI parameters for certain classes of targets such as coins in a beach or small gold nuggets in a stream bed or small nuggets in mineralized soil.
There is a limit to how much power you can pump into a target area as the doubling of detection distance in theory needs 64 times more power. That is 2 to the third power to stimulate the target and 2 to the third power for the return trip of the target eddies back to the coil which adds up to 2 to the sixth power or 64. Then there is minimizing noise in the RX circuit when using the highest gain to maximize sensitivity. Here is where Eric Foster integrated many RX pulses to lower the noise level much like what is used in Lock-in amplifiers.
I hope this helps?
Joseph J. Rogowski
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