In geometry, a rhombohedron (also called a rhombic hexahedron or, inaccurately, a rhomboid) is a special case of a parallelepiped in which all six faces are congruent rhombi. It can be used to define the rhombohedral lattice system, a honeycomb with rhombohedral cells. A rhombohedron has two opposite apices at which all face angles are equal; a prolate rhombohedron has this common angle acute, and an oblate rhombohedron has an obtuse angle at these vertices. A cube is a special case of a rhombohedron with all sides square.

Special cases

The common angle at the two apices is here given as θ {\displaystyle \theta } . There are two general forms of the rhombohedron: oblate (flattened) and prolate (stretched).

In the oblate case θ > 90 {\displaystyle \theta >90^{\circ }} and in the prolate case θ < 90 {\displaystyle \theta <90^{\circ }} . For θ = 90 {\displaystyle \theta =90^{\circ }} the figure is a cube.

Certain proportions of the rhombs give rise to some well-known special cases. These typically occur in both prolate and oblate forms.

Solid geometry

For a unit (i.e.: with side length 1) rhombohedron, with rhombic acute angle θ   {\displaystyle \theta ~} , with one vertex at the origin (0, 0, 0), and with one edge lying along the x-axis, the three generating vectors are

e1 : ( 1 , 0 , 0 ) , {\displaystyle {\biggl (}1,0,0{\biggr )},}
e2 : ( cos θ , sin θ , 0 ) , {\displaystyle {\biggl (}\cos \theta ,\sin \theta ,0{\biggr )},}
e3 : ( cos θ , cos θ cos 2 θ sin θ , 1 3 cos 2 θ 2 cos 3 θ sin θ ) . {\displaystyle {\biggl (}\cos \theta ,{\cos \theta -\cos ^{2}\theta \over \sin \theta },{{\sqrt {1-3\cos ^{2}\theta 2\cos ^{3}\theta }} \over \sin \theta }{\biggr )}.}

The other coordinates can be obtained from vector addition of the 3 direction vectors: e1 e2 , e1 e3 , e2 e3 , and e1 e2 e3 .

The volume V {\displaystyle V} of a rhombohedron, in terms of its side length a {\displaystyle a} and its rhombic acute angle θ   {\displaystyle \theta ~} , is a simplification of the volume of a parallelepiped, and is given by

V = a 3 ( 1 cos θ ) 1 2 cos θ = a 3 ( 1 cos θ ) 2 ( 1 2 cos θ ) = a 3 1 3 cos 2 θ 2 cos 3 θ   . {\displaystyle V=a^{3}(1-\cos \theta ){\sqrt {1 2\cos \theta }}=a^{3}{\sqrt {(1-\cos \theta )^{2}(1 2\cos \theta )}}=a^{3}{\sqrt {1-3\cos ^{2}\theta 2\cos ^{3}\theta }}~.}

We can express the volume V {\displaystyle V} another way :

V = 2 3   a 3 sin 2 ( θ 2 ) 1 4 3 sin 2 ( θ 2 )   . {\displaystyle V=2{\sqrt {3}}~a^{3}\sin ^{2}\left({\frac {\theta }{2}}\right){\sqrt {1-{\frac {4}{3}}\sin ^{2}\left({\frac {\theta }{2}}\right)}}~.}

As the area of the (rhombic) base is given by a 2 sin θ   {\displaystyle a^{2}\sin \theta ~} , and as the height of a rhombohedron is given by its volume divided by the area of its base, the height h {\displaystyle h} of a rhombohedron in terms of its side length a {\displaystyle a} and its rhombic acute angle θ {\displaystyle \theta } is given by

h = a   ( 1 cos θ ) 1 2 cos θ sin θ = a   1 3 cos 2 θ 2 cos 3 θ sin θ   . {\displaystyle h=a~{(1-\cos \theta ){\sqrt {1 2\cos \theta }} \over \sin \theta }=a~{{\sqrt {1-3\cos ^{2}\theta 2\cos ^{3}\theta }} \over \sin \theta }~.}

Note:

h = a   z {\displaystyle h=a~z} 3 , where z {\displaystyle z} 3 is the third coordinate of e3 .

The body diagonal between the acute-angled vertices is the longest. By rotational symmetry about that diagonal, the other three body diagonals, between the three pairs of opposite obtuse-angled vertices, are all the same length.

Relation to orthocentric tetrahedra

Four points forming non-adjacent vertices of a rhombohedron necessarily form the four vertices of an orthocentric tetrahedron, and all orthocentric tetrahedra can be formed in this way.

Rhombohedral lattice

The rhombohedral lattice system has rhombohedral cells, with 6 congruent rhombic faces forming a trigonal trapezohedron:

See also

  • Lists of shapes

Notes

References

External links

  • Weisstein, Eric W. "Rhombohedron". MathWorld.
  • Volume Calculator https://rechneronline.de/pi/rhombohedron.php

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