You basically compiled a list of second-order effects, which make you loose the sight of the first-order effect. The mass of the tonearm as a whole is not negligible when compared to the mass of the soundbox alone, to begin with. If you don't set - first of all - the resonance of the needle compliance / tonearm mass in an area in which such resonance won't give sound colorations / interference cancellations / tracking issues, all other lesser tweakings will be to no avail.Inigo wrote: Mon Oct 17, 2022 2:30 pm I see your point, Marco. But in the well known Wilson's electrical circuit equivalent to the soundbox, the soundbox and tonearm are not represented. It has been my long time idea to try to fit these elements in the circuit, to understand their role. No success yet, but some thoughts about it are clear to me. And one is this: whatever the link in the circuit, the soundbox mass is the second reaction the needle vibration finds in its path to the diaphragm, the first being the resistance to bending as felt from the short end of the needlebar. But the needlebar is supported on the soundbox, and some vibration will escape to the soundbox mass through the fulcrum supports. Here, the first reaction it finds is the inertia of the soundbox to vibration, and this is precisely its mass, as felt from the needle point. Further in that signal escape path, we have the compliance of the soundbox rubber neck, the mass of the tonearm, the compliance of the tonearm bearing, and the mass of the machine.
Changing a heavy soundbox with a much lighter one in which the compliance has not been changed accordingly, will unavoidably lead to disappointing results.