Let denote the Packing Density, which is the fraction of a Volume filled by identical packed Spheres. In 2-D (Circle Packing), there are two periodic packings for identical Circles: square lattice and hexagonal lattice. Fejes Tóth (1940) proved that the hexagonal lattice is indeed the densest of all possible plane packings (Conway and Sloane 1993, pp. 8-9).
In 3-D, there are three periodic packings for identical spheres: cubic lattice, face-centered cubic lattice, and hexagonal lattice. It was hypothesized by Kepler in 1611 that close packing (cubic or hexagonal) is the densest possible (has the greatest ), and this assertion is known as the Kepler Conjecture. The problem of finding the densest packing of spheres (not necessarily periodic) is therefore known as the Kepler Problem. The Kepler Conjecture is intuitively obvious, but the proof remained elusive until it was accomplished in a series of papers by Hales culminating in 1998. Gauß (1831) proved that the face-centered cubic is the densest lattice packing in 3-D (Conway and Sloane 1993, p. 9). This result has since been extended to Hypersphere Packing.
In 3-D, face-centered cubic close packing and hexagonal close packing (which is distinct from hexagonal lattice), both give
(1) |
(2) |
``Random'' close packing in 3-D gives only (Jaeger and Nagel 1992).
The Packing Densities for several packing types are summarized in the following table.
Packing | (exact) | (approx.) |
square lattice (2-D) | 0.7854 | |
hexagonal lattice (2-D) | 0.9069 | |
cubic lattice | 0.5236 | |
hexagonal lattice | 0.6046 | |
face-centered cubic lattice | 0.7405 | |
random | -- | 0.6400 |
For cubic close packing, pack six Spheres together in the shape of an Equilateral Triangle and place another Sphere on top to create a Triangular Pyramid. Now create another such grouping of seven Spheres and place the two Pyramids together facing in opposite directions. A Cube emerges. Consider a face of the Cube, illustrated below.
The ``unit cell'' cube contains eight -spheres (one at each Vertex) and six
Hemispheres. The total Volume of Spheres in the unit cell is
(3) |
(4) |
(5) |
Hexagonal close packing must give the same values, since sliding one sheet of Spheres cannot affect the
volume they occupy. To verify this, construct a 3-D diagram containing a hexagonal unit cell with three layers. Both the top
and the bottom contain six -Spheres and one Hemisphere. The total number of spheres in these
two rows is therefore
(6) |
(7) |
(8) |
(9) |
(10) |
If we had actually wanted to compute the Volume of Sphere inside and outside the Hexagonal
Prism, we could use the Spherical Cap equation to obtain
(11) | |||
(12) |
The rigid packing with lowest density known has (Gardner 1966). To be Rigid, each Sphere must touch at least four others, and the four contact points cannot be in a single Hemisphere or all on one equator.
If spheres packed in a cubic lattice, face-centered cubic lattice, and hexagonal lattice are allowed to expand, they form cubes, hexagonal prisms, and rhombic dodecahedra. Compressing a random packing gives polyhedra with an average of 13.3 faces (Coxeter 1958, 1961).
For sphere packing inside a Cube, see Goldberg (1971) and Schaer (1966).
See also Cannonball Problem, Circle Packing, Dodecahedral Conjecture, Hemisphere, Hermite Constants, Hypersphere, Hypersphere Packing, Kepler Conjecture, Kepler Problem, Kissing Number, Local Density, Local Density Conjecture, Sphere
References
Sphere Packings
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© 1996-9 Eric W. Weisstein