A twisted antiprism is obtained from an antiprism by rotating its top face by or ; it has a nontrivial infinitesimal isometric deformation. The case of the twisted triangular antiprism is known as Wunderlich's (or Schoenhardt's) octahedron. According to the Blaschke–Liebmann theorem, four nonadjacent faces of an infinitesimally flexible octahedron meet at a point. It seems that the theorem can be extended to the twisted antiprisms.

Let be any triangular face of the twisted antiprism, where and are on the bottom face and is on the top face. The rotation about the axis preserves the lengths of the sides of the triangle. If this rotation is done for all the triangles, the top face remains an equilateral triangle. Its side length is a function of the rotation angle , and the derivative of that function at is 0.

Let be a polyhedron with triangular faces and vertex set . An infinitesimal isometric deformation of is a map such that

at

for all edges of [3, definition 2.1].

This condition is equivalent to .

A polyhedron is infinitesimally flexible if it has an infinitesimal isometric deformation in which some of its dihedral angles change.

A theorem of Blaschke and Liebmann states: Let be a polyhedron combinatorially isomorphic to the octahedron. Color the faces of black and white so that each pair of adjacent faces has different colors. Then is infinitesimally flexible if and only if the four black faces intersect at a point, or equivalently, if the four white faces intersect at a point. Intersection points can lie at infinity [3, theorem 2.8].

References

[1] P. R. Cromwell, Polyhedra, Cambridge: Cambridge University Press, 1997 pp. 222–223.

[2] M. Goldberg, "Unstable Polyhedral Structures," Mathematics Magazine, 51, 1978 pp. 165–170.

[3] I. Izmestiev, "Examples of infinitesimally Flexible 3-dimensional Hyperbolic Cone-Manifolds," Journal of the Mathematical Society of Japan, 63(2), 2011 pp. 363–713. projecteuclid.org/euclid.jmsj/1303737798.