"These analogies between cartridge loading and automobile technology have their limitations."
In the old days before digital computers automotive companies use to model their suspension designs with analog circuits using inductors, capacitors and resistors. In the spring/mass system energy sloshes back and forth between the kinetic energy of the moving mass and the potential energy of the spring. In the electrical analog energy sloshes back and forth between the electric field in the capacitor and the magnetic field of the inductor. In the mechanical system the resonance is damped with a shock absorber, in the electrical circuit the resonance is damped with a resistor. Both systems are governed by the same differential equations. So the analogy is very apt.
The fact of the matter is a cartridge has inductance and forms a resonance tank in combination with the input and cable capacitance. The resonance peak will occur at a very high frequency, well beyond the audio band. Depending on the Q of the resonance you will see a rising frequency response well down in frequency from the peak. The Q of a resonance is determined by the source resistance of the cartridge and any load resistance. Now I will readily admit that if your phono pre is susceptible to RFI and your cart. is undamped, RFI will excite this resonance and raise all hell. That said, if your phono pre is not susceptible to RFI the resonance will still be there and the rising high end response it causes.
MC cartridges also have mechanical resonances that with some cart. need to be damped with a load resistor. Think speaker resonances and a low source impedance (high damping factor) amplifier.
But look, if you like the sound of your cart. running it wide open then go for it. Just don't make some kind of religion out of it.
In the old days before digital computers automotive companies use to model their suspension designs with analog circuits using inductors, capacitors and resistors. In the spring/mass system energy sloshes back and forth between the kinetic energy of the moving mass and the potential energy of the spring. In the electrical analog energy sloshes back and forth between the electric field in the capacitor and the magnetic field of the inductor. In the mechanical system the resonance is damped with a shock absorber, in the electrical circuit the resonance is damped with a resistor. Both systems are governed by the same differential equations. So the analogy is very apt.
The fact of the matter is a cartridge has inductance and forms a resonance tank in combination with the input and cable capacitance. The resonance peak will occur at a very high frequency, well beyond the audio band. Depending on the Q of the resonance you will see a rising frequency response well down in frequency from the peak. The Q of a resonance is determined by the source resistance of the cartridge and any load resistance. Now I will readily admit that if your phono pre is susceptible to RFI and your cart. is undamped, RFI will excite this resonance and raise all hell. That said, if your phono pre is not susceptible to RFI the resonance will still be there and the rising high end response it causes.
MC cartridges also have mechanical resonances that with some cart. need to be damped with a load resistor. Think speaker resonances and a low source impedance (high damping factor) amplifier.
But look, if you like the sound of your cart. running it wide open then go for it. Just don't make some kind of religion out of it.