Examples of groups
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Some elementary examples of groups in mathematics are given on Group (mathematics). Further examples are listed here.
Permutations of a set of three elements
Consider three colored blocks (red, green, and blue), initially placed in the order RGB. Let a be the operation "swap the first block and the second block", and b be the operation "swap the second block and the third block".
We can write xy for the operation "first do y, then do x"; so that ab is the operation RGB → RBG → BRG, which could be described as "move the first two blocks one position to the right and put the third block into the first position". If we write e for "leave the blocks as they are" (the identity operation), then we can write the six permutations of the three blocks as follows:
 e : RGB → RGB
 a : RGB → GRB
 b : RGB → RBG
 ab : RGB → BRG
 ba : RGB → GBR
 aba : RGB → BGR
Note that aa has the effect RGB → GRB → RGB; so we can write aa = e. Similarly, bb = (aba)(aba) = e; (ab)(ba) = (ba)(ab) = e; so every element has an inverse.
By inspection, we can determine associativity and closure; note in particular that (ba)b = bab = b(ab).
Since it is built up from the basic operations a and b, we say that the set {a,b} generates this group. The group, called the symmetric group S_{3}, has order 6, and is nonabelian (since, for example, ab ≠ ba).
The group of translations of the plane
A translation of the plane is a rigid movement of every point of the plane for a certain distance in a certain direction. For instance "move in the NorthEast direction for 2 miles" is a translation of the plane. Two translations such as a and b can be composed to form a new translation a ∘ b as follows: first follow the prescription of b, then that of a. For instance, if
 a = "move NorthEast for 3 miles"
and
 b = "move SouthEast for 4 miles"
then
 a ∘ b = "move to bearing 8.13° for 5 miles" (bearing is measured counterclockwise and from East)
Or, if
 a = "move to bearing 36.87° for 3 miles" (bearing is measured counterclockwise and from East)
and
 b = "move to bearing 306.87° for 4 miles" (bearing is measured counterclockwise and from East)
then
 a ∘ b = "move East for 5 miles"
(see Pythagorean theorem for why this is so, geometrically).
The set of all translations of the plane with composition as operation forms a group:
 If a and b are translations, then a ∘ b is also a translation.
 Composition of translations is associative: (a ∘ b) ∘ c = a ∘ (b ∘ c).
 The identity element for this group is the translation with prescription "move zero miles in whatever direction desired".
 The inverse of a translation is given by walking in the opposite direction for the same distance.
This is an abelian group and our first (nondiscrete) example of a Lie group: a group which is also a manifold.
The symmetry group of a square: dihedral group of order 8
Dih_{4} as 2D point group, D_{4}, [4], (*4•), order 4, with a 4fold rotation and a mirror generator. 
Dih_{4} in 3D dihedral group D_{4}, [4,2]^{+}, (422), order 4, with a vertical 4fold rotation generator order 4, and 2fold horizontal generator 
Groups are very important to describe the symmetry of objects, be they geometrical (like a tetrahedron) or algebraic (like a set of equations). As an example, we consider a glass square of a certain thickness (with a letter "F" written on it, just to make the different positions discriminable).
In order to describe its symmetry, we form the set of all those rigid movements of the square that don't make a visible difference (except the "F"). For instance, if an object turned 90° clockwise still looks the same, the movement is one element of the set, for instance a. We could also flip it horizontally so that its underside becomes its top side, while the left edge becomes the right edge. Again, after performing this movement, the glass square looks the same, so this is also an element of our set and we call it b. A movement that does nothing is denoted by e.
Given two such movements x and y, it is possible to define the composition x ∘ y as above: first the movement y is performed, followed by the movement x. The result will leave the slab looking like before.
The point is that the set of all those movements, with composition as operation, forms a group. This group is the most concise description of the square's symmetry. Chemists use symmetry groups of this type to describe the symmetry of crystals and molecules.
Generating the group
Let's investigate our squares symmetry group some more. Right now, we have the elements a, b and e, but we can easily form more: for instance a ∘ a, also written as a^{2}, is a 180° degree turn. a^{3} is a 270° clockwise rotation (or a 90° counterclockwise rotation). We also see that b^{2} = e and also a^{4} = e. Here's an interesting one: what does a ∘ b do? First flip horizontally, then rotate. Try to visualize that a ∘ b = b ∘ a^{3}. Also, a^{2} ∘ b is a vertical flip and is equal to b ∘ a^{2}.
We say that elements a and b generate the group.
This group of order 8 has the following Cayley table:
∘  e  b  a  a^{2}  a^{3}  ab  a^{2}b  a^{3}b 

e  e  b  a  a^{2}  a^{3}  ab  a^{2}b  a^{3}b 
b  b  e  a^{3}b  a^{2}b  ab  a^{3}  a^{2}  a 
a  a  ab  a^{2}  a^{3}  e  a^{2}b  a^{3}b  b 
a^{2}  a^{2}  a^{2}b  a^{3}  e  a  a^{3}b  b  ab 
a^{3}  a^{3}  a^{3}b  e  a  a^{2}  b  ab  a^{2}b 
ab  ab  a  b  a^{3}b  a^{2}b  e  a^{3}  a^{2} 
a^{2}b  a^{2}b  a^{2}  ab  b  a^{3}b  a  e  a^{3} 
a^{3}b  a^{3}b  a^{3}  a^{2}b  ab  b  a^{2}  a  e 
For any two elements in the group, the table records what their composition is.
Here we wrote "a^{3}b" as a shorthand for a^{3} ∘ b.
In mathematics this group is known as the dihedral group of order 8, and is either denoted Dih_{4}, D_{4} or D_{8}, depending on the convention. This was an example of a nonabelian group: the operation ∘ here is not commutative, which can be seen from the table; the table is not symmetrical about the main diagonal.
.
Normal subgroup
This version of the Cayley table shows that this group has one normal subgroup shown with a red background. In this table r means rotations, and f means flips. Because the subgroup is normal, the left coset is the same as the right coset.
e  r_{1}  r_{2}  r_{3}  f_{v}  f_{h}  f_{d}  f_{c}  

e  e  r_{1}  r_{2}  r_{3}  f_{v}  f_{h}  f_{d}  f_{c} 
r_{1}  r_{1}  r_{2}  r_{3}  e  f_{c}  f_{d}  f_{v}  f_{h} 
r_{2}  r_{2}  r_{3}  e  r_{1}  f_{h}  f_{v}  f_{c}  f_{d} 
r_{3}  r_{3}  e  r_{1}  r_{2}  f_{d}  f_{c}  f_{h}  f_{v} 
f_{v}  f_{v}  f_{d}  f_{h}  f_{c}  e  r_{2}  r_{1}  r_{3} 
f_{h}  f_{h}  f_{c}  f_{v}  f_{d}  r_{2}  e  r_{3}  r_{1} 
f_{d}  f_{d}  f_{h}  f_{c}  f_{v}  r_{3}  r_{1}  e  r_{2} 
f_{c}  f_{c}  f_{v}  f_{d}  f_{h}  r_{1}  r_{3}  r_{2}  e 
The elements e, r_{1}, r_{2}, and r_{3} form a subgroup, highlighted in red (upper left region). A left and right coset of this subgroup is highlighted in green (in the last row) and yellow (last column), respectively. 
Free group on two generators
The free group with two generators a and b consists of all finite strings that can be formed from the four symbols a, a^{−1}, b and b^{−1} such that no a appears directly next to an a^{−1} and no b appears directly next to a b^{−1}. Two such strings can be concatenated and converted into a string of this type by repeatedly replacing the "forbidden" substrings with the empty string. For instance: "abab^{−1}a^{−1}" concatenated with "abab^{−1}a" yields "abab^{−1}a^{−1}abab^{−1}a", which gets reduced to "abaab^{−1}a". One can check that the set of those strings with this operation forms a group with neutral element the empty string ε := "". (Usually the quotation marks are left off; this is why the symbol ε! is required)
This is another infinite nonabelian group.
Free groups are important in algebraic topology; the free group in two generators is also used for a proof of the Banach–Tarski paradox.
The set of maps
The sets of maps from a set to a group
Let G be a group and S a nonempty set. The set of maps M(S, G) is itself a group; namely for two maps f,g of S into G we define fg to be the map such that (fg)(x) = f(x)g(x) for every x∈S and f^{−1} to be the map such that f^{−1}(x) = f(x)^{−1}.
Take maps f, g, and h in M(S, G). For every x in S, f(x) and g(x) are both in G, and so is (fg)(x). Therefore, fg is also in M(S, G), or M(S, G) is closed. For ((fg)h)(x) = (fg)(x)h(x) = (f(x)g(x))h(x) = f(x)(g(x)h(x)) = f(x)(gh)(x) = (f(gh))(x), M(S, G) is associative. And there is a map i such that i(x) = e where e is the unit element of G. The map i makes all the functions f in M(S, G) such that if = fi = f, or i is the unit element of M(S, G). Thus, M(S, G) is actually a group.
If G is commutative, then (fg)(x) = f(x)g(x) = g(x)f(x) = (gf)(x). Therefore, so is M(S, G).
Automorphism groups
Groups of permutations
Let G be the set of bijective mappings of a set S onto itself. Then G forms a group under ordinary composition of mappings. This group is called the symmetric group, and is commonly denoted , Σ_{S}, or . The unit element of G is the identity map of S. For two maps f and g in G are bijective, fg is also bijective. Therefore, G is closed. The composition of maps is associative; hence G is a group. S may be either finite or infinite.
Matrix groups
If n is some positive integer, we can consider the set of all invertible n by n matrices over the reals, say. This is a group with matrix multiplication as operation. It is called the general linear group, GL(n). Geometrically, it contains all combinations of rotations, reflections, dilations and skew transformations of ndimensional Euclidean space that fix a given point (the origin).
If we restrict ourselves to matrices with determinant 1, then we get another group, the special linear group, SL(n). Geometrically, this consists of all the elements of GL(n) that preserve both orientation and volume of the various geometric solids in Euclidean space.
If instead we restrict ourselves to orthogonal matrices, then we get the orthogonal group O(n). Geometrically, this consists of all combinations of rotations and reflections that fix the origin. These are precisely the transformations which preserve lengths and angles.
Finally, if we impose both restrictions, then we get the special orthogonal group SO(n), which consists of rotations only.
These groups are our first examples of infinite nonabelian groups. They are also happen to be Lie groups. In fact, most of the important Lie groups (but not all) can be expressed as matrix groups.
If this idea is generalised to matrices with complex numbers as entries, then we get further useful Lie groups, such as the unitary group U(n). We can also consider matrices with quaternions as entries; in this case, there is no welldefined notion of a determinant (and thus no good way to define a quaternionic "volume"), but we can still define a group analogous to the orthogonal group, the symplectic group Sp(n).
Furthermore, the idea can be treated purely algebraically with matrices over any field, but then the groups are not Lie groups.
For example, we have the general linear groups over finite fields. The group theorist J. L. Alperin has written that "The typical example of a finite group is , the general linear group of n dimensions over the field with q elements. The student who is introduced to the subject with other examples is being completely misled."^{ [1]}
See also
References
 ^ Alperin, Jonathan L. (1984). "Book Review: Finite groups". Bulletin of the American Mathematical Society. New Series. 10: 121–124. doi: 10.1090/S027309791984152108.