In the early 1960's in Australia, Zephyr seemingly sold many of the type 130M mumetal cased microphone transformer. I appear to have four of these units, although they are not marked with a model number. I've started to measure their performance for MC step-up applications, as they can provide either +20dB, +24dB or +28dB gain. With the secondary loaded by 47k with 150pF shunt, the raw frequency response shows a +4dB high frequency peak out at 33kHz, which is flattened with an added shunt 39k+330pF RC to give a nominal -3dB bandwidth from 10Hz to 45kHz. The 24dB and 20dB connections have similar bandwidth, although the added RC requires tweaking for similar flat responses
The impedance spectrum seen from the primary winding is nominally 50 ohm, as anticipated by the advertised specs. Similarly the other connections present nominal 100 and 300 ohm midband.
The frequency spectrum was generated by a PicoScope 4224A using FRA4PicoScope software, with a 10mVpk sine driving primary directly from the scope signals output. The 150pF shunt loading comprised 57+17=74pF from the 1:1 probe and scope input, along with an added 68pF ceramic. The software can smooth out the noise, but only from 10Hz and above, so the plot is a little ragged, and there is no incentive to raise the drive signal level. The signal generator of the scope has a 600 ohm rated output resistance. I'm unsure how much influence the generator's output resistance would have on the character of the frequency spectrum - any thoughts?
The impedance spectrum was generated by REW software and an EMU 0404 USB soundcard and calibrated test jig. The added RC on the secondary winding influences the higher frequency character of that impedance plot, and contributes significantly to the dip in impedance in the 3k to 20k region. Any thoughts on how much of an influence the varying impedance would be, and whether it could be flattened along with also keeping a flat secondary frequency response ?
I'll play around a little more over the coming days.
Ciao, Tim
The impedance spectrum seen from the primary winding is nominally 50 ohm, as anticipated by the advertised specs. Similarly the other connections present nominal 100 and 300 ohm midband.
The frequency spectrum was generated by a PicoScope 4224A using FRA4PicoScope software, with a 10mVpk sine driving primary directly from the scope signals output. The 150pF shunt loading comprised 57+17=74pF from the 1:1 probe and scope input, along with an added 68pF ceramic. The software can smooth out the noise, but only from 10Hz and above, so the plot is a little ragged, and there is no incentive to raise the drive signal level. The signal generator of the scope has a 600 ohm rated output resistance. I'm unsure how much influence the generator's output resistance would have on the character of the frequency spectrum - any thoughts?
The impedance spectrum was generated by REW software and an EMU 0404 USB soundcard and calibrated test jig. The added RC on the secondary winding influences the higher frequency character of that impedance plot, and contributes significantly to the dip in impedance in the 3k to 20k region. Any thoughts on how much of an influence the varying impedance would be, and whether it could be flattened along with also keeping a flat secondary frequency response ?
I'll play around a little more over the coming days.
Ciao, Tim