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Covariant Differentiation
Book chapter

Covariant Differentiation

Introduction to Tensor Analysis and the Calculus of Moving Surfaces, pp 105-132
10 Aug 2013

Abstract

Covariant Derivative Legitimate Definition Riemann-Christoffel Tensor Tensor Properties Vanishing Christoffel Symbols
Chapter 6 demonstrated that the tensor property is the key to invariance. However, a partial derivative \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $$\partial /\partial {Z}^{i}$$ \end{document} of a tensor is itself not a tensor. This is a major obstacle in the way of developing differential geometry using the coordinate approach. For example, the expression \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $$\partial {T}^{i}/\partial {Z}^{i}$$ \end{document} cannot be used as a definition of divergence since it evaluates to different values in different coordinates. Similarly, \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $${Z}^{ij}{\partial }^{2}T/\partial {Z}^{i}\partial {Z}^{j}$$ \end{document} is not invariant and is therefore not a legitimate definition of the Laplacian.

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