Symmetry plays a very important role in nature and there is certainly no exception
at the atomic scale. Atoms themselves are highly symmetric (spheres) and most of the molecules
and all crystalline materials have some elements of symmetry - centers (inversion),
axes (rotation), planes (reflection), translation and a general combination of them all.
For example, a spiral; a fascinating feature of the DNA molecule,
is a combination of rotation around and translation along the symmetry axis.
Each molecule is assigned to a certain point group: a set of symmetry elements which can be applied to this molecule. Completely asymmetric molecules belong to the group C1, which has only one symmetry element: identity (E). Obviously, all other molecules have identity as well and thus all point groups have element E present.
Here are some examples of well known small molecules which have symmetry:
Water (C2v)
Benzene (D6h )
Methane (Td )
Hydrogen (D∞h )
The water molecule (H2O) has four symmetry elements: identity (E), 2nd order axis of symmetry (C2) and two symmetry planes (?v). Higher symmetry molecules, such as benzene (C6H6) and methane (CH4), have more elements of symmetry. Methane has five and benzene has twelve different elements of symmetry, while the total number of symmetry elements: twenty four - is equal for both molecules. Hydrogen, a linear molecule with two equivalent atoms, has an infinite number of symmetry elements such as rotations (C2and C∞), rotation-reflections (S∞) and planes (Cv).
Carbon, the major element in organic molecules, can form linear polymers (such as hydrocarbons (CnHm), two-dimensional sheets (graphite) and three-dimensional crystals (diamond). Fullerenes and nanotubes, which are very popular in nanotechnology research, are also made from carbon as pictured below:
Hydrocarbon
Graphite
Diamond
Fullerene
Nanotube
Crystals, macroscopic periodic systems, made from atoms and molecules have fascinating symmetry, which in combination with color is a working horse of the big industry sector - jewelry.
There are fourteen 3D crystal lattices with different symmetries (Bravais lattices): which are characterized by the relations between unit cell parameters and the presence of the additional lattice point in the center of the unit cell or on its faces. See below:
Primitive(P)
Body-centered(I)
Side-centered(C)
Face-centered(F)
There are seven crystal systems which have one or more different types of unite cell (P, I,C, or F):