Yes. Offhand I can think of two ways to give theoretical figures for ideal, unloaded boards (OK, just one). If you think of triangles, it's easy. [n] is the span, [r] is the radius, [e] is the elevation at the center: e=r-sqrt(r^2-[n/2]^2) For a circle it's the same. The general equation is (y-y_0)^2+(x-x_0)^2=r^2 If the span, or chord is [-n/2<=x<=n/2)], you might want its ends to be at [y=0]: y_0=-sqrt(r^2-(n/2)^2) (note the minus sign) The equation for the circle becomes y=sqrt(r^2-x^2)-sqrt(r^2-(n/2)^2); it follows that at the center, for [x=0], y=r-sqrt(r^2-(n/2)^2)=e (identical to the solution with triangles) For arc length - in this case the width of the curved panel where it is attached to a crowned rib with a chord length [n]: l_a=r*asin(n/r) Of course, none of this applies to real materials. ;) Clark
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