Hi Mike... You have to sort of put 6 and 6 together if you are just using the Wogram article to get to the equalized speed of sound. Start off with the fact that sound moves many times faster along the grain then across in an unribbed panel because moduli of elasticity in the two directions are in a ratio of approximately 20:1 (anisotropic) . We can discern from that that in general, adding stiffness will increase the speed of sound through wood regardless of orientation. (because /v/=root(Y/d) in solids) Throw in the fact that by equalizing the stiffness of the board across the grain one also equalizes the speed sound propagates in either direction and that if you dont do the former (which consequents in the latter) then "effective vibrating area is reduced and the radiation efficiency is decreased over a broad frequency band." And you arrive at the assumption that it is the need for a homogenous anisotropic relationship in general that is what is desired. And that by definition includes the speed of sound. Seems kind of self evident elstwize that if sound is moving at highly reduced rate of speed in what is essentially half the board you are going to limit the boards ability to radiate sound efficiently. You are effectively just letting it vibrate (significantly) in one direction yes ?? over simplified but more or less correct I believe. Otherwise.. this has been presented several times in several places before in the archives and other places. My point was that it seems possible that one can compensate for the panels anisotrophism independent of any structural requirements by laminating a panel much like crowned laminated ribs are constructed and running the grain of such a soundboard perpendicular to the bridge. Ribs in such a configuration could be used primarilly for such a compenation since the need for crown support would be much less then in a conventional board. At least... thats where my musing on the idea has taken me at this point. Cheers RicB *Michael Spalding writes:* Ric, I've never understood the importance of sound travelling through the soundboard parallel to the grain and across the grain. When we "hear" a piano, we're sensing air pressure differences, which are created by the diaphragmatic movements of the board. Wogram states clearly in the excerpts you provided, that the ribs are there to equalize the stiffness of the board across and parallel to the grain, to optimise the diaphragmatic response. He says nothing about the speed of sound transmission throught the wood, at least in the excerpts provided. Where does this idea come from?
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