The limited frequency range may be a problem though. You may not properly see the resonance peak, which may be a problem (or not).marcus4audio said:Yes, nothing fancy but it works http://gsmserver.com/shop/equipment/measuring_equipment/multimeter_mastech/digital_multimeter_mastech_my64.phpIs it battery-powered?
Pls see attached.This part I still can't figure out. maybe I have a problem to visualize the connections and therms. I still don't understand what is Z in this situation :/ any drawing please ?In the "almost perfect" region, the impedance Z is equal to sqrt[Rdc²+(2pi.F.L)]. At LF, the DCR is dominant, but as frequency increases, the impedance gets much higher than DCR, then you can use L=Z/2pi.F as a very good approximation.
You should draw a graph of Z vs. frequency, with a log scales.
You can see clearly the DCR-controlled part (parallel to the X-axis), the L.omega part (6dB/octave) and the resonance peak.
You have to experiment with the value of R. You must make sure that at any frequency you wish to measure the inductor, R is at least 10x larger than the impedance.
Starting with a rough estimate, let's say 1mH, at 20kHz Z is 125 ohms, so you can use 2k, which will give you a measured voltage of .6V at 20kHz, about 30mV at 1kHz, and probably a few millivolts at 20Hz, depending on the DCR of the inductor.