I gave you the formula on how to calculate the spring of whatever kind. The indicator for a succesfull decoupling frequency, to put it a bit sloppy, is how much the spring(s) sinks in when loaded with the speaker. 1mm is way uber-sufficient given the current gravitation constant of mother earth. All other parameters cancel each other out (math).I wouldn't take it personally.
I tried to read your post 292 again, but as soon as I hit :
Another is the elasticity of a spike. Everything becomes soft,,,,,
I start giggling and can not read the rest, perhaps if you re-post it and put that clause right at the end.
In short: take a mousepad, upused if you wil, done! For very small speakers: support only the edges, right?
Don't you call it "spike" over there, but "cone"? Whatever, yes, the tip of that thing is weaker than you might think. And if it were not, the surface it contacts isn't material stolen from a neutron star. At least if they say so, it would be a relatively new lie.
I neglected rotational modes, but some qualitative and semi-quantative arguments relate the spring idea to rotation and shift also. The caveat with the analogy to piles / piers in cities doesn't count because it doen't take those arguments into account. It is empty, caveat emptor. I'm not so much convinced that even the most basic ideas of physics would help you all here.
Btw, you cannot decouple using a heavy concrete slab against a wobbly floor, and so on and on.