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What Is Symmetry?

In geometry, an object exhibits symmetry if it looks the same after a transformation, such as reflection or rotation. Symmetry is the underlying mathematical principle behind all patterns and is important in art (used in architecture, pottery, quilting and rug making), mathematics (relating to geometry, group theory and linear algebra), biology (in shapes of organisms), chemistry (in shapes of molecules and crystal structures), and physics (where symmetries correspond to conserved quantities). The word "symmetry" is a 16th-century Latin derivative from the Greek words for "together" (syn-) and "measure" (metron).

Types of symmetry


In general usage, symmetry most often refers to mirror or reflective symmetry; that is, a line (in 2-D) or plane (in 3-D) can be drawn through an object such that the two halves are mirror images of each other. An isosceles triangle and a human face are examples. Mathematically, an object that exhibits mirror symmetry is said to be “invariant under reflection,” meaning reflecting the object in a certain way doesn’t change its appearance. 

An isosceles triangle and a butterfly are examples of objects that exhibit reflective symmetry. Objects in 2-D have a line of symmetry; objects in 3-D have a plane of symmetry. They are invariant under reflection. (Image credit: Robert J. Coolman Lightspring Shutterstock)

In biology, reflective symmetry is often referred to as bilateral symmetry, as found in mammals, reptiles, birds and fish.


Another form of symmetry commonly found in biology is radial symmetry. It is found in flowers and many sea creatures, such as sea anemones, sea stars and jellyfish. Mathematically, such objects are described as exhibiting rotational symmetry, for being “invariant under rotation.” Such objects have a point (in 2-D) or an axis (in 3-D) about which an object can be rotated some amount and remain invariant.

A yin-yang symbol and a pinwheel are examples of objects that exhibit rotational symmetry. Objects in 2-D have a center of symmetry; objects in 3-D have an axis of symmetry. They are invariant under rotation. (Image credit: Svitlana Amelina Jessmine Shutterstock


If imagined to extend for infinity in all directions, a 2-D or 3-D pattern can exhibit translational symmetry, for being “invariant under translation.” All tessellations, many jungle gyms and most patterns found on rugs and wallpaper exhibit translational symmetry.

Wallpaper designs and jungle gyms are examples of patterns that exhibit translational symmetry. If extended to infinity in all directions, they are invariant under translation. (Image credit: Tiax KPG_Payless Shutterstock)

Other forms of symmetry

While there are examples of objects that exhibit more than one type of symmetry (for example a six-pointed star exhibits six lines of reflection and a point of 6-fold rotation), there are some objects and patterns that are invariant only under two transformations done at the same time.

(Image credit: Robert J. Coolman

Improper Rotation = Reflection + Rotation

A pentagonal antiprism with directional edges is invariant under improper rotation (in the example above, rotation by a tenth of a circle, and reflected across a horizontal plane).

(Image credit: Robert J. Coolman

Glide Reflection = Translation + Reflection

A footprint pattern like the above example, if extended to infinity in either direction, is invariant under glide reflection (a translation combined with a reflection).

(Image credit: Robert J. Coolman

Screw Rotation = Translation + Rotation

A helix made of tetrahedrons, if extended to infinity in either direction, is invariant under screw rotation (in this example, a translation combined with a rotation of 131.8 degrees).

Categorizing objects and patterns

Mathematicians and crystallographers categorize an object’s or pattern’s symmetry according to the variety of ways it can be transformed and still remain invariant. A 2-D or 3-D object is assigned a "point group" to indicate all the ways it can remain invariant under reflection and rotation (and in 3-D, improper rotation). When using an object as a pattern motif, it is convenient to assign it to one of the crystallographic point groups: in 2-D, there are 10 of these (shown below); in 3-D, there are 32.

The ten crystallographic point groups in 2-D. (Image credit: Robert J. Coolman)

In common notation, called Schoenflies notation after Arthur Moritz Schoenflies, a German mathematician:

  • “C” stands for “cyclic.” These objects have rotational symmetry, but no reflective symmetry. The number indicates what-fold rotational symmetry they have, so the symbol labeled C2 has two-fold symmetry, for example. All cyclic shapes have a mirror image that “spins the other way.”
  • “D” stands for “dihedral.” These objects have both reflective and rotational symmetry. The number indicates what-fold rotational symmetry they have as well as the number of lines of symmetry.


A lattice is a repeating pattern of points in space where an object can be repeated (or more precisely, translated, glide reflected, or screw rotated). In 1-D there’s just one lattice, in 2-D there are five, and in 3-D there are 14.

To make a pattern, a 2-D object (which will have one of the 10 crystallographic point groups assigned to it) is repeated along a 1-D or 2-D lattice. A 2-D object repeated along a 1-D lattice forms one of seven frieze groups. A 2-D object repeated along a 2-D lattice forms one of 17 wallpaper groups.

3-D patterns are more complicated, and are rarely found outside of crystallography. The various 3-D point groups repeated along the various 3-D lattices form 230 varieties of space group. 3-D objects can also be repeated along 1-D or 2-D lattices to produce rod groups or layer groups, respectively.


Also important is invariance under a fourth kind of transformation: scaling. Concentric circles of geometrically progressing diameter are invariant under scaling. When an object is invariant under a specific combination of translation, reflection, rotation and scaling, it produces a new kind of pattern called a fractal.

The Koch curve, if extended to infinity both inward and outward, is invariant under a specific procedure of translation, rotation, and scaling. (Image credit: Robert J. Coolman)

Additional resources

Robert Coolman

Robert Coolman, PhD, is a teacher and a freelance science writer and is based in Madison, Wisconsin. He has written for Vice, Discover, Nautilus, Live Science and The Daily Beast. Robert spent his doctorate turning sawdust into gasoline-range fuels and chemicals for materials, medicine, electronics and agriculture. He is made of chemicals.