6 Differential Geometry

In differential geometry, it is convention to generalize tangent vectors as to a differential operator.

6.1 Elementary Example

6.1.1 Simple

At a point \(P\), tangent vectors are expanded in a finite basis of the tangent space.

\[ T_{P}M = \operatorname{span}\{ e_{1},\ e_{2} \} \]

\[ v = v^{1} e_{1} + v^{2} e_{2} \]

where

  • \(T_{P}M\) is the tangent space at \(P\).
  • \(e_{1}, e_{2}\) are basis tangent vectors.
  • \(v^{1}, v^{2}\) are components of \(v\).