Integers Let be the
additive group of the integers, {{math|1=
Z = ({..., −2, −1, 0, 1, 2, ...}, +)}} and the subgroup {{math|1=(3
Z, +) = ({..., −6, −3, 0, 3, 6, ...}, +)}}. Then the cosets of in are the three sets , , and , where . These three sets partition the set , so there are no other right cosets of . Due to the
commutativity of addition and . That is, every left coset of is also a right coset, so is a normal subgroup. (The same argument shows that every subgroup of an Abelian group is normal.) This example may be generalized. Again let be the additive group of the integers, {{math|1=
Z = ({..., −2, −1, 0, 1, 2, ...}, +)}}, and now let be the subgroup {{math|1=(
mZ, +) = ({..., −2
m, −
m, 0,
m, 2
m, ...}, +)}}, where is a positive integer. Then the cosets of in are the sets , , ..., , where . There are no more than cosets, because . The coset is the
congruence class of modulo . The subgroup is normal in , and so, can be used to form the quotient group the group of
integers mod.
Vectors Another example of a coset comes from the theory of
vector spaces. The elements (vectors) of a vector space form an
abelian group under
vector addition. The
subspaces of the vector space are
subgroups of this group. For a vector space , a subspace , and a fixed vector in , the sets \{\mathbf{x} \in V \mid \mathbf{x} = \mathbf{a} + \mathbf{w}, \mathbf{w} \in W\} are called
affine subspaces, and are cosets (both left and right, since the group is abelian). In terms of 3-dimensional
geometric vectors, these affine subspaces are all the "lines" or "planes"
parallel to the subspace, which is a line or plane going through the origin. For example, consider the
plane . If is a line through the origin , then is a subgroup of the abelian group . If is in , then the coset is a line parallel to and passing through .
Matrices Let be the multiplicative group of matrices, G = \left \{\begin{bmatrix} a & 0 \\ b & 1 \end{bmatrix} \colon a, b \in \R, a \neq 0 \right\}, and the subgroup of , H= \left \{\begin{bmatrix} 1 & 0 \\ c & 1 \end{bmatrix} \colon c \in \mathbb{R} \right\}. For a fixed element of consider the left coset \begin{align} \begin{bmatrix} a & 0 \\ b & 1 \end{bmatrix} H = &~ \left \{\begin{bmatrix} a & 0 \\ b & 1 \end{bmatrix}\begin{bmatrix} 1 & 0 \\ c & 1 \end{bmatrix} \colon c \in \R \right\} \\ =&~ \left \{\begin{bmatrix} a & 0 \\ b + c & 1 \end{bmatrix} \colon c \in \mathbb{R}\right\} \\ =&~ \left \{\begin{bmatrix} a & 0 \\ d & 1 \end{bmatrix} \colon d \in \mathbb{R}\right\}. \end{align} That is, the left cosets consist of all the matrices in having the same upper-left entry. This subgroup is normal in , but the subgroup T= \left \{\begin{bmatrix} a & 0 \\ 0 & 1 \end{bmatrix} \colon a \in \mathbb{R} - \{0\} \right\} is not normal in . == As orbits of a group action ==