Tangent space

In mathematics, the tangent space of a manifold facilitates the generalization of vectors from affine spaces to general manifolds, since in the latter case one cannot simply subtract two points to obtain a vector that gives the displacement of the one point from the other. In mathematics, the tangent space of a manifold facilitates the generalization of vectors from affine spaces to general manifolds, since in the latter case one cannot simply subtract two points to obtain a vector that gives the displacement of the one point from the other. In differential geometry, one can attach to every point x {displaystyle x} of a differentiable manifold a tangent space—a real vector space that intuitively contains the possible directions in which one can tangentially pass through x {displaystyle x} . The elements of the tangent space at x {displaystyle x} are called the tangent vectors at x {displaystyle x} . This is a generalization of the notion of a bound vector in a Euclidean space. The dimension of the tangent space at every point of a connected manifold is the same as that of the manifold itself. For example, if the given manifold is a 2 {displaystyle 2} -sphere, then one can picture the tangent space at a point as the plane that touches the sphere at that point and is perpendicular to the sphere's radius through the point. More generally, if a given manifold is thought of as an embedded submanifold of Euclidean space, then one can picture a tangent space in this literal fashion. This was the traditional approach toward defining parallel transport and was used by Dirac. More strictly, this defines an affine tangent space, which is distinct from the space of tangent vectors described by modern terminology. In algebraic geometry, in contrast, there is an intrinsic definition of the tangent space at a point of an algebraic variety V {displaystyle V} that gives a vector space with dimension at least that of V {displaystyle V} itself. The points p {displaystyle p} at which the dimension of the tangent space is exactly that of V {displaystyle V} are called non-singular points; the others are called singular points. For example, a curve that crosses itself does not have a unique tangent line at that point. The singular points of V {displaystyle V} are those where the ‘test to be a manifold’ fails. See Zariski tangent space. Once the tangent spaces of a manifold have been introduced, one can define vector fields, which are abstractions of the velocity field of particles moving in space. A vector field attaches to every point of the manifold a vector from the tangent space at that point, in a smooth manner. Such a vector field serves to define a generalized ordinary differential equation on a manifold: A solution to such a differential equation is a differentiable curve on the manifold whose derivative at any point is equal to the tangent vector attached to that point by the vector field. All the tangent spaces of a manifold may be ‘glued together’ to form a new differentiable manifold with twice the dimension of the original manifold, called the tangent bundle of the manifold. The informal description above relies on a manifold's ability to be embedded into an ambient vector space R m {displaystyle mathbb {R} ^{m}} so that the tangent vectors can ‘stick out’ of the manifold into the ambient space. However, it is more convenient to define the notion of a tangent space based solely on the manifold itself.