Hi Taff and Alexander,
As Taff mentioned, there are various ways to manipulate an icosahedron
to create geodesic spheres or domes. The so-called class I, method 1
described in Dome Book 2 by Joe Clinton and company, and also by Hugh
Kenner in his book, Geodesic Math and How to Use It, is very useful as
a starting point of dome design, as are other methods. But because
each builder, each building method, and each building application has
its own requirements and peculiarities, it seems to me like a good
idea to adapt any given geodesic geometry to fit the actual need.
Even-frequency class I, method 1 domes sit flat at the equator. But
this is not the case for other potentially useful truncations such as
those just above and below the equator. For example, the 4/9ths and
5/9ths truncations (also called 3/8ths and 5/8ths) of the 3-frequency
icosahedral sphere do not sit flat. The same is true of the 5/12ths
and 7/12ths truncations of the 4-frequency icosa. Buckminster Fuller
produced 3- and 4-frequency dome designs that do indeed sit flat at
the truncations immediately above and below the equator, as well as at
the equator itself. But he didn’t publicly describe the math behind
it.
In the early 1970s, a mathematics teacher from Wisconsin, USA, named
David Kruschke, used spherical trigonometry to demonstrate Fuller’s
level-base method for both 3 and 4 frequency domes. The chord factors
in his little publication, called Dome Cookbook of Geodesic Geometry
(first published in 1972, with another edition in 1975, but now out of
print) are still used today by various dome manufacturers because of
the obvious advantages of having all base-level vertices lie exactly
in the same plane. Kruschke mentions his reasons for publishing this
work. In the preface of his booklet he writes: “Unlike Domebook One
and Domebook Two, the chord factor results here are in close agreement
with Buckminster Fuller’s (a fact that is important when one is
working with three frequency domes....). Oddly enough, this confusion
and this book would have been unnecessary if Fuller would have
published his derivations.”
For comparison, here are the chord factors, to 5 decimal places, for
class I, method 1 (i.e., Clinton, Domebook 2, Kenner, Rick Bono’s
Windome program, and the Desert Domes website) and for the Fuller-
Kruschke layouts.
Class I, method 1:
3v icosa: 0.34862, 0.40355, 0.41241
4v icosa: 0.25318, 0.29524, 0.29453, 0.31287, 0.32492, 0.29859
Fuller & Kruschke:
3v icosa: 0.32971, 0.38229, 0.44106, 0.42149
4v icosa: 0.22219, 0.25958, 0.30906, 0.31287, 0.32492, 0.32942
In the case of the 3v icosa, the level base of the Fuller-Kruschke
design comes at a price: there is an extra chord factor (strut length)
to deal with and three triangle types instead of two.
As for the 4v icosa, the Fuller-Kruschke design has the same number of
chord factors (6) and the same number of triangle types (6). Two of
the triangle types are mirror-image scalene triangles (but otherwise
identical), which can slow down work in the shop. As I said, the main
advantage of this design is that the base is level at three useful
truncations: 5/12, 6/12 and 7/12.
But why stop there? It's possible to further simplify the design (and
fabrication) by (1) getting rid of ALL the scalene triangles, which
reduces the number of triangle types from 6 to 5, and (2) reducing the
number of unique edge lengths from 6 to 4 – at the same time
maintaining a level base at the 5/12ths and 7/12ths truncations (but
not at the equator).
Here are the new chord factors (4 instead of 6):
0.23766, 0.27741, 0.32611, 0.31405.
With this set of chord factors, Taff, there is indeed an increase in
the ratio of longest strut length to shortest. But it’s pretty small.
The ratio is 1.372 compared with 1.283 for the Class I, method 1 dome.
But it’s less than the ratio for the Fuller-Kruschke design, namely
1.483.
Most of the triangles in this alternative layout are quite close to
equilateral and I think the resulting dome would be aesthetically
pleasing. But so far I’ve only modeled it mathematically, in Excel
using the spherical coordinate system, not in any CAD program like
SketchUp. I’ve uploaded a jpg image to the files section. It shows
which strut goes where. File: 4v-icosa-solution3c-level-base.jpg.
Solution 3c is just one of several potentially practical triangle
layouts that stray from the conventional Clinton-Kenner geometry, the
Fuller-Kruschke geometry, and the electric-charge-repulsion
distribution of points that Taff uses. This “pretzel-twisting”, with
fabrication efficiency in mind, can be applied to other parent
polyhedra (e.g., octahedon) and other frequencies (I’ve done it with
5v, 6v and 9v), as well as class II dome layouts.
Any feedback on this will be most welcome.
Cheers,
Gerry in Quebec
> Note that you can download a copy of "Domebook 2" here:
http://groups.google.com/group/geodesichelp/browse_thread/thread/5176...
>
> Regards,
> Taff