Typical MC resistance is a few ohms (say 5) so 6n8 gives a time constant of a bout 34ns, and a corner frequency of maybe 5MHz, so miles from having any effect in audio band.
MC inductance varies over a wide range depending on type; Hagerman suggests between 5uH and 5mH.
This mean there are potentially two different frequency scales to consider ( or a frequency and a damping factor). The L/R time constant depends on the load resistance, and for 500R (470 close enough for hand waving) would range between 10ns (5uH/500) and 10us (5mH/500), corresponding to 16MHz through 16KHz. So only for the highest inductance types (I guess high output ones) will the resistive loading roll off the treble.
The LC resonant frequency is given by 1/(2 pi sqrt( LC)) . Using the example range above for L and 6n8 for C, you frequencies ranging from 860KHz to 28kHz for the high inductance case.
The picture is further complicated by some MC designs having a massive ultrasonic resonance, which may want taming, while others are intrinsically flat.
I think the conclusion has got to be that each model needs its own loading, and that in many cases much bigger capacitances may be needed, up to as much as a uF in extreme cases.