I have now hundreds of screenshots showing the frequency responses of various pickups when they are excited by a low impedance coil.
For obvious reasons, these curves can vary according to...
-the capacitance of the cable used;
-the strength of the signal sent to the pickup;
-the volume of the guitar input which collects the signal sent by the pickup;
-the external hardware involved: pots and their value, added wiring and its capacitance, covers...
Most of the time, I can "duplicate" these physical measurements through a 5Spice simulation.
BUT there's ONE thing that I don't understand: why, with some pickups, does the extreme high range rolls off abruptly while its decay remains smooth with other pickups?
To show what I mean, here is a quadruple screenshot showing the response, under variable conditions, of 4 PU's:

The response of the P90 has roughly the shape of a triangle. You would see the same shape if I showed you the response of a Duncan SH55, Gibson Burstbucker or Gibson T-Top.
BUT with the Duncan APH1, SH1 and PG1 tested in my picture above, you can see how the high frequencies die above 12 or 15khz. You'd notice the same thing with a Jackson J50BC, for example...
This phenomenon doesn't appear to depend on magnets (Alnico 5 or 2 as well as ceramic in the examples above). It doesn't appear to depend on baseplates either, nor on wiring insulation, slugs or screw poles, which are roughly the same in vastly different frequency response screenshots but which differ enormously in some other pu's whose response has the same shape...
WHAT is for you the cause of this behaviour (= tendency of some PU's to roll off the extreme highrange), knowing that I've "excited" each pickup from its "screw poles" coil (the frequency response would be different if measured from the "slug poles" bobbin)?
Could it depend on wax potting, for example?
Thx in advance for any documented answer. :-)
For obvious reasons, these curves can vary according to...
-the capacitance of the cable used;
-the strength of the signal sent to the pickup;
-the volume of the guitar input which collects the signal sent by the pickup;
-the external hardware involved: pots and their value, added wiring and its capacitance, covers...
Most of the time, I can "duplicate" these physical measurements through a 5Spice simulation.
BUT there's ONE thing that I don't understand: why, with some pickups, does the extreme high range rolls off abruptly while its decay remains smooth with other pickups?
To show what I mean, here is a quadruple screenshot showing the response, under variable conditions, of 4 PU's:
The response of the P90 has roughly the shape of a triangle. You would see the same shape if I showed you the response of a Duncan SH55, Gibson Burstbucker or Gibson T-Top.
BUT with the Duncan APH1, SH1 and PG1 tested in my picture above, you can see how the high frequencies die above 12 or 15khz. You'd notice the same thing with a Jackson J50BC, for example...
This phenomenon doesn't appear to depend on magnets (Alnico 5 or 2 as well as ceramic in the examples above). It doesn't appear to depend on baseplates either, nor on wiring insulation, slugs or screw poles, which are roughly the same in vastly different frequency response screenshots but which differ enormously in some other pu's whose response has the same shape...
WHAT is for you the cause of this behaviour (= tendency of some PU's to roll off the extreme highrange), knowing that I've "excited" each pickup from its "screw poles" coil (the frequency response would be different if measured from the "slug poles" bobbin)?
Could it depend on wax potting, for example?
Thx in advance for any documented answer. :-)
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