Originally posted by simonbaker
View Post
Probably on three frequencies around the resonance frequency:
Fr-BW/2, Fr, Fr+BW/2,
where Fr = resonance frequency and BW = bandwidth (few 100 Hz).
But not decided yet. I will see this, if I made a field test.
BTW, I can increase the coil voltage up to +/-3V (6Vpp) until it gets clipped by the sound card. Using differential mode, I can process up to +/- 6V (12 Vpp) coil voltage. It is interesting, that very small changes in the amplitude and phase shift are sufficient enough to make this detector with mono coil possible. The current hardware consumes only 4.25 mA at 9V. So a 9V battery block can last for a long period.
The new coil is finished but not shielded yet. I have taken 5 strands of magnet wire, each 0.3 mm diameter. So the finished coil has ca. 20,6 cm mean diameter, 12 mm bundle thickness, 2x37 turns (74 turns total), 2.2 mH inductivity and a resistance of 1.8 Ohm total. It has a center tap and is operated in fully differential mode (differential stimulation, differential sensing). The difference is made digitally in the software of course.
Aziz

). No more adjustments necessary. Very simple design.
Leave a comment: