Thanks Teres for elaborating. Guess it's a good thing you feel your product development results have affirmed the theoretical reasoning which preceded them :-)
On somewhat of a sidetrack note, let me toss out a bit of theoretical reasoning of my own. I think almost everbody in the business could have it backwards in placing substantial platter mass out near the rim. I know why it's done, but suspect that in a different sense it might be a disease worse than the cure. IMO it could be much better from a resonance standpoint to concentrate whatever mass is required for inertial effect as close to the bearing axis as possible and make the outer regions as light as practical. I understand this would entail use of greater mass overall if one wanted to achieve an equivalent inertial effect. But locating mass very far away from its point of mechanical constraint (the main bearing) is inviting trouble in my estimation. Given that a platter must have a flat top, I think maybe a parabolically-curved underside, yielding a constantly varying thickness, might work well...something like this half-profile:
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(Sorry, the system doesn't permit the full illustration without justifying it, so imagine it mirrored with the bearing axis at the left margin.) Of course the bearing-point itself would be up inside the shape, slightly above its center of mass. Looking at this, I wonder if possibly the York TT that Fremer has sometimes pictured in his column might not have a similar platter profile, but I don't really know and can't think another myself. But if it does, that makes more sense to me than the common approaches. End of off-topic musings...
On somewhat of a sidetrack note, let me toss out a bit of theoretical reasoning of my own. I think almost everbody in the business could have it backwards in placing substantial platter mass out near the rim. I know why it's done, but suspect that in a different sense it might be a disease worse than the cure. IMO it could be much better from a resonance standpoint to concentrate whatever mass is required for inertial effect as close to the bearing axis as possible and make the outer regions as light as practical. I understand this would entail use of greater mass overall if one wanted to achieve an equivalent inertial effect. But locating mass very far away from its point of mechanical constraint (the main bearing) is inviting trouble in my estimation. Given that a platter must have a flat top, I think maybe a parabolically-curved underside, yielding a constantly varying thickness, might work well...something like this half-profile:
__________________________________________________
________________________________________________
______________________________________
____________________________
____________________
______________
__________
________
_______
(Sorry, the system doesn't permit the full illustration without justifying it, so imagine it mirrored with the bearing axis at the left margin.) Of course the bearing-point itself would be up inside the shape, slightly above its center of mass. Looking at this, I wonder if possibly the York TT that Fremer has sometimes pictured in his column might not have a similar platter profile, but I don't really know and can't think another myself. But if it does, that makes more sense to me than the common approaches. End of off-topic musings...