Vector addition 2026-10-14
Vector addition is the vector space operation combining two vectors into their sum. It is commutative and associative, has the zero vector as identity, and distributes with scalar multiplication as specified by the vector space axioms. Coordinatewise addition describes it after choosing a basis.
Vector space Created 2026-09-24 Updated 2026-10-14
A vector space over a field is a set equipped with vector addition and scalar multiplication satisfying the vector space axioms. Its vectors can represent directed displacements, lists of measurements, polynomials, or entire functions. The common structure is that adding two elements and multiplying an element by a scalar remain meaningful operations inside the same space.
For example, uses coordinatewise addition and scaling. With
we have . Moving twice along and once along reaches the same vector as five horizontal and four vertical steps. The two descriptions refer to different bases of the same space. A basis makes such descriptions unique; a spanning set makes them possible.
Figure 1.
The same vector has coordinates 5,4 in the Cartesian basis and 2,1 in an oblique basis
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The space of real polynomials of degree at most two has basis : the polynomial is the linear combination with coordinates . The zero vector here is the zero polynomial, and addition combines coefficients. A derivative is a linear map on this space; its matrix records how it acts on the three basis vectors. The same coordinate machinery therefore handles both geometric motion and operations on functions.
The choice of field matters. The complex numbers form a one-dimensional vector space over with basis , but a two-dimensional vector space over with basis . The question "how many independent directions?" has an answer only after the allowed scalars are specified. Likewise, polynomials of degree exactly two do not form a vector space: subtraction can remove the leading term, and the zero polynomial is absent.
The usefulness of the abstraction is that a linear map is determined by its values on a basis. Once those images are known, linear combinations give its action on every vector. The rank-nullity theorem relates the number of attainable outputs to the number of invisible input directions, while change of basis lets us choose coordinates suited to the problem. Eigenvectors, for example, choose directions on which repeated application of a linear operator becomes scalar multiplication.
A historical source is Hermann Grassmann's Die lineale Ausdehnungslehre (1844). Its full title advertises applications to other branches of mathematics, statics, mechanics, magnetism and crystallography; the original edition is digitized by ETH-Bibliothek. This gives an early setting for treating geometric quantities algebraically across different applications, rather than attributing the modern axiom list to that title alone.[ref]
Vector space axioms 2026-10-14
Addition makes an Abelian group: for all , and , there is a zero vector , and every has an additive inverse . Scalar multiplication satisfies, for ,
Both operations take values in . These requirements make manipulating linear combinations independent of how sums are grouped or expanded.
Vector subspace Created 2026-09-24 Updated 2026-10-14
A vector subspace is a nonempty subset of a vector space closed under vector addition and scalar multiplication, and is therefore itself a vector space. Equivalently, whenever belong to the subset, so does for all allowed scalars . In particular it contains the zero vector.
For example, the plane is a vector subspace, with basis . Indeed every element is . The parallel plane misses the zero vector and is an affine subspace instead. Homogeneous constraints produce vector subspaces: is the kernel of the linear map . This lets us describe all solutions of a homogeneous linear equation through a basis of its kernel.
Zero vector 2026-10-14
The zero vector of a vector space is its additive identity: for every vector . It is unique, because if is another such identity then . Distributivity gives , so after cancellation. In a coordinate vector space it has every coordinate zero.