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Geodesic Coordinate Transformation 📂Geometry

Geodesic Coordinate Transformation

Definition1

Let’s define UR2U \subset \mathbb{R}^{2} as an open set. Define x:UR3\mathbf{x} : U \to \mathbb{R}^{3} as a coordinate chart that satisfies the following:

g11=1andg12=g21=0 g_{11} = 1 \quad \text{and} \quad g_{12} = g_{21} = 0

[gij]=[100g22] \left[ g_{ij} \right] = \begin{bmatrix} 1 & 0 \\ 0 & g_{22} \end{bmatrix}

In this case, gijg_{ij} is the coefficient of the first fundamental form. Such x\mathbf{x} is called a geodesic coordinate chart.
{} For a surface MM, if there is a curve γ:[a,b]M\gamma : [a,b] \to M that satisfies γ([a,b])x(U)\gamma\left( [a,b] \right) \subset \mathbf{x}\left( U \right) and is a u2u^{2}-curve of x\mathbf{x}, then x\mathbf{x} is called the geodesic coordinate chart along γ\boldsymbol{\gamma}.


  1. Richard S. Millman and George D. Parker, Elements of Differential Geometry (1977), p115 ↩︎