Post by antigua on Sept 25, 2016 19:48:04 GMT -5
Vs.
Ken Willmott sent me some GFS Nashville Filter'tron style humbuckers, PAF clones that attempt to resemble Filter'trons with a metal cover than has that characteristic H hole in the top. I happen to have Fender Fideli'trons sitting loose, so I decided to you them as a point of contrast, since Fender Fideli'trons appear to be very good Filter'tron stand-ins. The GFS Nashville go for about $35, while the Fender Fideli's go for about $50 used apiece.
After taking a look, the GFS appear to be PAF clones with plastic spacers and ceramic magnets, so that leads one to think they will sound like a bright PAF, not a Filter'tron, but it turns out, that if the GFS is wire in parallel rather than series, it does get a resonant peak that is very close. GFS also loads the Nashvilles with a ceramic bar, which helps approximate the double tall AlNiCo bar of a Filter'tron.
Electrical Differences
Here is a plot that shows how the Fideli'trons compare to the GFS if the GFS are wired in series. The two higher peaks are the GFS bridge and neck in series, while the two lower peaks are the Fideli'tron, which is always in series. The GFS Nashvilles have a lower treble response, and much higher output than the Fender Fideli'trons.
In this configuration, the Fender Fideli'trons produce 2.3H and 1.8H inductance for the bridge and neck, while the GFS Nashvilles produce 6.6H and 4.3H inductance, very different levels of output.
But if the GFS are wired in parallel, they come very close together. In parallel, the GFS' now have inductances of 1.6H and 1.1H for the bridge and neck, which is lower than the Fideli'trons wired in series. The GFS' still have a lower peak despite the lower inductance, which indicates a higher degree of parasitic capacitance is at work, since the resonant peak becomes lower whenever either the inductance, or the capacitance, is increased.
Of course, this is unloaded, as though there were no volume or tone pots complicating matters, so here is the same plot above, but this time with the simulated effects of a guitar cable and volume and tone pots, by way of 200k ohms resistance and 470pF capacitance across the pickups:
Now, all of the sudden, the GFS Nashville's have a higher peak than the Fideli'trons interestingly, and this is because the GFS had a higher parasitic capacitance to begin with, and so the added 470pF capacitance didn't drag their peak frequencies down as far.
The GFS Nashville's still have a higher Q factor than the Fideli'trons, but that's nothing a little working of the tone knob on the guitar wouldn't correct for.
These plots are all made with the covers grounded, so the capacitive coupling between the coils and the covers and base plates, as well as the conductor cable, are all baked into the results.
Here are some raw numbers:
GFS Nashville Vintage Filtertron Style Bridge Humbucker R02
DC Resistance:
- series: 9.46K
- b/w coil: 4.71K
- r/g coil: 4.75K
Inductance:
- series: 6.598H
- parallel: 1.631H
- b/w coil: 2.940H
- r/g coil: 2.933H
GFS Nashville Vintage Filtertron Style Neck Humbucker R01
DC Resistance:
- series: 8.37K
- b/w coil: 4.13K
- r/g coil: 4.24K
Inductance:
- series: 4.323H
- parallel: 1.086H
- b/w coil: 1.801H
- r/g coil: 1.800H
Fender Fideli'tron Bridge
DC Resistance in Series: 5.13K
Inductance in Series: 2.325H
Fender Fideli'tron Neck
DC Resistance in Series: 4.46K
Inductance in Series: 1.7853H
Physical Differences
The other big aspect to consider is the magnets. Unlike PAFs, Filter'trons have a larger AlNiCo 5 magnet inside them, giving them a higher flux density than a PAF. I measure PAFs at around 230 Gauss at the screw/pole tops, while the Fender Fideli'trons measure closer to 300 gauss.
The GFS Nashville's meet this difference by using a ceramic bar magnet, and this causes the gauss at the GFS' screw tops shoot past the Fideli'tron to 320 to 350 gauss.
The higher flux density means more current, and more voltage for a given degree of string movement, as well as subtle tonal differences that are hard to pinpoint, owing to the exponential rate at which magnetic flux decreases with the distance between the strings and the charged pole pieces. But I'm glad to see that GFS didn't skimp out on this particular detail.
Here are some pics of the guts:
GFS Nashville
Fender Fideli'tron
Setup details:
Bode plots are made with a Velleman PCSGU250 and the supplied probes in 10x mode, with the function generator feeding a driver coil of 0.48mH, placed on top of the pickup and driven with 2Vpp. The pickup is connected to an integrator circuit, designed by Ken Willmottkenwillmott.com/blog/, with a Velleman 10x probe, and fed back into the Velleman PCSGU250. I measured the probes' capacitance at 20pF, so that amount is subtracted from the capacitance calculation. The "loaded" tests have exactly 470k ohms and 200pF capacitance across the pickup.
The inductance and Q measurements are made with an Extech 380193 in "SER" series mode, and the mean value between the 1kHz and 120Hz modes is recorded. The capacitance value is derived from the inductance and measured resonant peak.
Magnets are tested with a Spin Doctor ERgravitastech.weebly.com/spin-doctor-er.html