Gram–Euler theorem explained

In geometry, the Gram–Euler theorem, Gram-Sommerville, Brianchon-Gram or Gram relation[1] (named after Jørgen Pedersen Gram, Leonhard Euler, Duncan Sommerville and Charles Julien Brianchon) is a generalization of the internal angle sum formula of polygons to higher-dimensional polytopes. The equation constrains the sums of the interior angles of a polytope in a manner analogous to the Euler relation on the number of d-dimensional faces.

Statement

Let

P

be an

n

-dimensional convex polytope. For each k-face

F

, with

k=\dim(F)

its dimension (0 for vertices, 1 for edges, 2 for faces, etc., up to n for P itself), its interior (higher-dimensional) solid angle

\angle(F)

is defined by choosing a small enough

(n-1)

-sphere centered at some point in the interior of

F

and finding the surface area contained inside

P

. Then the Gram–Euler theorem states:[2] [3] \sum_ (-1)^ \angle(F) = 0In non-Euclidean geometry of constant curvature (i.e. spherical,

\epsilon=1

, and hyperbolic,

\epsilon=-1

, geometry) the relation gains a volume term, but only if the dimension n is even:\sum_ (-1)^ \angle(F) = \epsilon^(1 + (-1)^n)\operatorname(P)Here,

\operatorname{Vol}(P)

is the normalized (hyper)volume of the polytope (i.e, the fraction of the n-dimensional spherical or hyperbolic space); the angles

\angle(F)

also have to be expressed as fractions (of the (n-1)-sphere).

When the polytope is simplicial additional angle restrictions known as Perles relations hold, analogous to the Dehn-Sommerville equations for the number of faces.

Examples

For a two-dimensional polygon, the statement expands into:\sum_ \alpha_v - \sum_e \pi + 2\pi = 0where the first term

A=style\sum\alphav

is the sum of the internal vertex angles, the second sum is over the edges, each of which has internal angle

\pi

, and the final term corresponds to the entire polygon, which has a full internal angle

2\pi

. For a polygon with

n

faces, the theorem tells us that

A-\pin+2\pi=0

, or equivalently,

A=\pi(n-2)

. For a polygon on a sphere, the relation gives the spherical surface area or solid angle as the spherical excess:

\Omega=A-\pi(n-2)

.

For a three-dimensional polyhedron the theorem reads:\sum_ \Omega_v - 2\sum_e \theta_e + \sum_f 2\pi - 4\pi = 0where

\Omegav

is the solid angle at a vertex,

\thetae

the dihedral angle at an edge (the solid angle of the corresponding lune is twice as big), the third sum counts the faces (each with an interior hemisphere angle of

2\pi

) and the last term is the interior solid angle (full sphere or

4\pi

).

History

The n-dimensional relation was first proven by Sommerville, Heckman and Grünbaum for the spherical, hyperbolic and Euclidean case, respectively.

See also

References

  1. Camenga. Kristin A.. 2006. Angle sums on polytopes and polytopal complexes. Cornell University. math/0607469 .
  2. Book: Grünbaum, Branko. Convex Polytopes. Convex Polytopes. October 2003. Springer. 978-0-387-40409-7. 297–303.
  3. Perles. M. A.. Shepard. G. C.. 1967. Angle sums of convex polytopes. Mathematica Scandinavica. 21. 2. 199–218. 10.7146/math.scand.a-10860. 24489707. 0025-5521. free.