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It starts with the cube expanded to the haptihedron and inverted into the Vector Equilibrium (VE). The following description helps to picture the missing link. Then add another layer of spheres nesting in the gaps between spheres in the first layer. The 92 spheres move for some reason and in some way and come to rest as an icosahedron. This can happen if the core sphere is removed or collapsed.
Recently, Todd Squires of Harvard University and Michael Brenner of MIT have proposed an explanation for some of the experimental results, incorporating hitherto overlooked effects of hydrodynamics. 1 Their model produces quantitative agreement with measurements, by Amy Larsen and David Grier at the University of Chicago, of the behavior of two colloidal particles near a single wall. 2 Hints of attraction A typical charge-stabilized latex colloidal suspension consists of spheres with diameters on the order of 1 mm or smaller, dispersed in water. Sulfate or other groups on the spheres dissociate in solution, producing a large surface charge density on the spheres. The spheres are surrounded by counterions that are many times more numerous and much smaller than the spheres.
The purpose of this article is to show how puzzles might be built using pieces from different angle systems along with pieces that are a combination of more than one system. Hopefully this opens up a new world of possibilities to be explored. Within each of these grids we can look at the possibilities of how three or four spheres might be attached together in order to make different puzzle pieces. It is the only possible mixed-angle piece built of three spheres. Their shapes are new to the puzzle connoisseur, despite the fact that they consist of combinations of only 3 or 4 elements.
For all our computations the index of refraction is fixed at a value 1. 005i, which is close to the refractive index of mineral tropospheric aerosols and was used in previous extensive studies of light scattering by spheroids and Chebyshev particles. For monodisperse bispheres with touching components in a fixed orientation, electromagnetic interactions between the constituent spheres result in a considerably more complicated interference structure in the scattering patterns than that for single monodisperse spheres. However, this increased structure is largely washed out by orientational averaging and results in scattering patterns for randomly oriented bispheres that are close to those for single spheres with size equal to the size of the bisphere components. Unlike other nonspherical particles such as cubes and spheroids, randomly oriented bispheres do not exhibit pronounced enhancement of side scattering and reduction of backscattering and positive polarization at side-scattering angles.

A site I really like: http://www.vs.afrl.af.mil/Factsheets/techsat21.html

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