Part 1 - Page 1

Rotational Tetrahedral Symmetry

Tetrahedra consists of four vertices which are all connected to each other by edges.  These edges form the sides of four equilateral triangles.  Since each vertex is connected to every other vertex by an edge the vertices can be arranged in any way and still have all the edges connecting the same vertices.

If a number is assigned to each vertex of a regular tetrahedron, any symmetry that maps the tetrahedron onto itself is easiliy represented as a permutation of the vertices.  A single transposition will be the equivalent to a reflection, as the orientation is reversed.   These reflection symmetries are discussed in the next part.  Below I show how any pair of transpositions is equivalent to a rotation about the center of the tetrahedron.  If the transpositions are disjoint, the rotation is about the line connecting the centers of the edges of the trasposed pairs.  If one of the vertices is fixed in both transpositions, the rotation is about the axis through that vertex.


Two disjoint transpositions represent a rotation of π about the axis through the midpoints of the edges that connect the transposed pairs.  Since these are disjoint, the order does not matter.

(12)(34)=(34)(12)


Two nondisjoint permutations represent a rotation of 3 about the axis through the fixed vertex.

(23)(34)=(234)


Reversing the order of the transpositions represents a rotation in the other direction, or a combination of two rotations in the original direction.  Thus it is also the inverse of a rotation in the opposite direction.

(34)(23)=(243)
(243)=(234)(234)
(234)(243)=(243)(234)=1


Note that the vertices used in the above rotations can be assigned in any manner and the symmetry will still be valid.


Part 1 - Page 2

Rotations

Rotational Tetrahedral Symmetry


At left are the seven elementary rotations. For ease of notation, I will define R12 to represent the rotation of π about the axis through the center of edge 12. This rotation then is equivalent to the permutation (12)(34). R13 and R14 are similarly defined.

R1 will represent a counter-clockwise rotation of 3 about the axis passing through vertex 1, facing the center through 1. This is equivalent to the permutation (234). R2, R3, and R4 will similarly represent the rotations about vertices 2, 3,and 4.

R12, R13, and R14 are their own inverses, so R122 = E. On the other hand, R1, ..., R4 all have order 3, so R12, ..., are also possible rotations.



These 11 rotations, along with the identity, represent all possible rotations of regular tetrahedra.  The group tables below show the possible permutation cycles of the vertices and the corresponding rotations.

  E R12 R13 R14 R12 R22 R32 R42 R1 R2 R3 R4
E E (12)(34) (13)(24) (14)(23) (243) (134) (142) (123) (234) (143) (124) (132)
 R12  (12)(34) E (14)(23) (13)(24) (142) (123) (243) (134) (132) (124) (143) (234)
R13 (13)(24) (14)(23) E (12)(34) (123) (142) (134) (243) (143) (234) (132) (124)
R14 (14)(23) (13)(24) (12)(34) E (134) (243) (123) (142) (124) (132) (234) (143)
R1 (234) (124) (132) (143) E (13)(24) (14)(23) (12)(34) (243) (142) (123) (134)
R2 (143) (132) (124) (234) (13)(24) E (12)(34) (14)(23) (123) (134) (243) (142)
R3 (124) (234) (143) (132) (14)(23) (12)(34) E (13)(24) (134) (123) (142) (243)
R4 (132) (143) (234) (124) (12)(34) (14)(23) (13)(24) E (142) (243) (134) (123)
R12 (243) (123) (134) (142) (234) (132) (143) (124) E (14)(23) (12)(34) (13)(24)
R22 (134) (142) (243) (123) (124) (143) (132) (234) (14)(23) E (13)(24) (12)(34)
R32 (142) (134) (123) (243) (132) (234) (124) (143) (12)(34) (13)(24) E (14)(23)
R42 (123) (243) (142) (134) (143) (124) (234) (132) (13)(24) (12)(34) (14)(23) E
  E R12 R13 R14 R12 R22 R32 R42 R1 R2 R3 R4
E E R12 R13 R14 R12 R22 R32 R42 R1 R2 R3 R4
R12 R12 E R14 R13 R32 R42 R12 R22 R4 R3 R2 R1
R13 R13 R14 E R12 R42 R32 R22 R12 R2 R1 R4 R3
R14 R14 R13 R12 E R22 R12 R42 R32 R3 R4 R1 R2
R1 R1 R3 R4 R2 E R13 R14 R12 R12 R32 R42 R22
R2 R2 R4 R3 R1 R13 E R12 R14 R42 R22 R12 R32
R3 R3 R1 R2 R4 R14 R12 E R13 R22 R42 R32 R12
R4 R4 R2 R1 R3 R12 R14 R13 E R32 R12 R22 R42
R12 R12 R42 R22 R32 R1 R4 R2 R3 E R14 R12 R13
R22 R22 R32 R12 R42 R3 R2 R4 R1 R14 E R13 R12
R32 R32 R22 R42 R12 R4 R1 R3 R2 R12 R13 E R14
R42 R42 R12 R32 R22 R2 R3 R1 R4 R13 R12 R14 E


Click here for a larger version of the tables.

These twelve permutations are clearly even permutations of four elements, and thus the set of rotations is isomorphic to A(4).

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Part 2 - Full Tetrahedral Symmmetry