Let MM be a and let π:TM→M\pi:TM\to M denote its .

Definition. A (smooth) vector field on MM is a smooth map X:M→TMX:M\to TM such that π∘X=idM\pi\circ X=\mathrm{id}_M. Equivalently, XX is a of the tangent bundle, assigning to each p∈Mp\in M a tangent vector

Xp∈TpMX_p \in T_pM

(where TpMT_pM is the ) in a way that is smooth in local coordinates.

A vector field can also be viewed as a derivation on smooth functions: for each XX and each f∈C∞(M)f\in C^\infty(M), one obtains a smooth function X(f)∈C∞(M)X(f)\in C^\infty(M) defined by differentiating ff in the direction XX. Using the pairing between tangent and cotangent spaces (see the ), this can be written pointwise as

(Xf)(p)=dfp(Xp).(Xf)(p)=df_p(X_p).

Given a F:M→NF:M\to N, the dFpdF_p transports tangent vectors, and when FF is a one can push vector fields forward along FF by applying dFdF pointwise.

Examples
  1. Coordinate vector fields on Rn\mathbb{R}^n. On M=RnM=\mathbb{R}^n with coordinates (x1,…,xn)(x^1,\dots,x^n), the vector field ∂/∂xi\partial/\partial x^i is defined by
    (∂∂xi)p(f)=∂(f∘x−1)∂xi∣x(p).\left(\frac{\partial}{\partial x^i}\right)_p(f)=\frac{\partial (f\circ x^{-1})}{\partial x^i}\bigg|_{x(p)}.
    More generally, any X=∑i=1nai(x) ∂/∂xiX=\sum_{i=1}^n a_i(x)\,\partial/\partial x^i with smooth coefficient functions aia_i is a smooth vector field.
  1. Radial and rotational fields on R2\mathbb{R}^2. In coordinates (x,y)(x,y), the radial field
    X=x ∂∂x+y ∂∂yX = x\,\frac{\partial}{\partial x}+y\,\frac{\partial}{\partial y}
    points outward from the origin, while the rotational field
    Y=−y ∂∂x+x ∂∂yY = -y\,\frac{\partial}{\partial x}+x\,\frac{\partial}{\partial y}
    generates counterclockwise rotation (away from the origin it is tangent to circles).
  1. Left-invariant vector fields on a Lie group. If GG is a , each element of the determines a unique by translating that tangent vector from the identity to every point via .