OK, this makes sense, except for the part concerning the piston movement, as - although I perfectly get your point - this is not what in mechano-acoustics is usually referred as "piston movement".Inigo wrote: Wed Nov 09, 2022 5:54 am Yes (structural engineer herein), the ridges provide stiffness in the circumferential direction (tangent) and flexibility in the radial direction. These ridges in the photo makes it easier for the center of the circumvented part, to do back-forth movement, like a piston.
A driver acting in piston-movement range is supposedly moving back and forth as a single, rigid unit. This happens for example with the cone of a woofer loudspeaker at low frequencies. I think that the shape of the ridges in picture, instead, would give more elasticity to the central part, which when excited by the needlebar would facilitate the creation of waves travelling from the center to the outer edge, rather than having the whole diaphragm moving more or less as a one-piece rigid body.
This is not anything necessarily bad, as confirmed by the fact that a flat diaphragm has been described as "poorly sounding". Also loudspeaker cones act as pistons only at lower frequencies; at higher frequencies, harmonic 2nd and higher order vibrations of the cone - that can have both circular nodal points as well as radial nodal points, that also combine with each other in very complex shapes - have an important role in sound emission, which actually gets of primary importance in wideband or full range speakers. The overall mass of the cone could never be moved as a single rigid unit at the speed needed to efficiently emit frequencies as high as 10 KHz, so the residual flexibility of the cone gains importance as the frequency gets higher.
This said, a cone is an inherently rigid shape by geometry, so it is relatively easy to have it acting like a piston, at least at low frequencies. Not so for a flat aluminium foil, obviously. Should you really want to experiment with a piston-moving diaphragm (perhaps you don't
