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I took a quick look at the last chapter, Rigid Tensegrities, of Part I of
Hugh Kenner's book. The illustrations contain very little detail, but the
text makes it clear that the "dips and gaps" of tensegrity structures are
reduced (as frequency increases) to the point where you can slide one 2x4
over another and bolt them together, with the tightened bolts serving as
the tensegrity tension members. This is the "just-kissing" contact Fuller
referred to in the passage you quoted. But there didn't seem to be enough
information in Kenner's book, at least for me, to be able to apply the
tensegrity equations to make an 8v rigid tensegrity. Taff is your best bet
for learning more about rigid tensegrities, nexorades, rotegrities.
.
On the topic of lesser-circle domes, where all vertices lie on the
spherical surface, I'm attaching a jpg of an 8v icosa dome layout (solution
5) that follows the general lines of the 8v Edwardsville dome, but not
exactly. Like that dome, the strut patterns are not fully triangulated --
it defines a set of hexagons, pentagons and triangles, rather than
triangles only. Removing the "omni-triangulation" restriction allows for
ALL pathways to be lesser circles, as I suspected.
In this dome, there's no ring of struts along the equator. If you "connect
the dots" along the equator, though, you'll see that the resulting pathway
undulates. However, the base of this dome, unlike that of the Edwardsville
rigid tensegrity, does not undulate. Ditto for the strut paths that mark
the perimeters of pentagons higher up.
- Gerry in Quebec
Here is solution 8e for the 6v icosa, class I. In this subdivision, a dome will sit flat at the 8/18, 9/18 (equator), and 10/18 truncations, but not at the 7/18 and 11/18 truncations. It is like the Fuller-Krushcke subdivision of the 4v icosa because the strut pathways one row of triangles above the equator and one row below form lesser circles, and the central pathway of struts exactly follows the equator (a great circle). It also has something in common with the Fuller-Kruschke 3v icosa: the angular distance between the parallel strut pathways just above and below the equator is 21.6246 degrees.
Taff, I've also attached a comma-delimited Excel file containing the Cartesian coordinates of the 28 vertices of the principal parent triangle.
- Gerry in Quebec
will produce the condition of "just-kissing" contact of the two-by-four ends of the islanded two-by-four chordal struts with the mid-girth contact points of one another.
| https://groups.google.com/d/topic/geodesichelp/SvgUIZepTfg/discussion |
| Topic: Econodome See Taff's post & attachment dated 10/30/15. Gerry in Québec |
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Hi Ashok, I have no plan on building a dome at that frequency.
The context was purely my love of modelling the different dome geometries in sketchup.
I only recently bothered to learn the kruschke method after coming across this thread. So then I modelled the lower frequencies up to what Gerry and Taff had done, and wanted to see what an 8v would give.
I will say I like "eveness" of the kruschke geometry. Would make it easier to insert doors, windows in a real world structure...
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Thanks Gerry,
Yes the 8v can't have a plane including the b struts on the pentagon edges.
I am guessing same for the 7v so as you say only 4 planes.
I will get to the 7v. I am just getting my head around solving the 5v with trig because before, to get going, I just copied a strut from what you & Taff had done. I can't imagine doing it iteratively via construction - so much work - but, it wouldn't surprise me if Taff saw a shortcut...
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Ashok, there are many here before me use sketchup....
The only one now missing between frequencies 3 and 8 is the 7v, which I guess has 4 parallel truncation planes....