Geodesic Coordinate Transformation
Definition1
Let’s define $U \subset \mathbb{R}^{2}$ as an open set. Define $\mathbf{x} : U \to \mathbb{R}^{3}$ as a coordinate chart that satisfies the following:
$$ g_{11} = 1 \quad \text{and} \quad g_{12} = g_{21} = 0 $$
$$ \left[ g_{ij} \right] = \begin{bmatrix} 1 & 0 \\ 0 & g_{22} \end{bmatrix} $$
In this case, $g_{ij}$ is the coefficient of the first fundamental form. Such $\mathbf{x}$ is called a geodesic coordinate chart.
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For a surface $M$, if there is a curve $\gamma : [a,b] \to M$ that satisfies $\gamma\left( [a,b] \right) \subset \mathbf{x}\left( U \right)$ and is a $u^{2}-$curve of $\mathbf{x}$, then $\mathbf{x}$ is called the geodesic coordinate chart along $\boldsymbol{\gamma}$.
Richard S. Millman and George D. Parker, Elements of Differential Geometry (1977), p115 ↩︎