Christoffel Symbols Explained: Uses & Definition

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SUMMARY

Christoffel symbols, denoted as ##\Gamma^{k}{}{}_{ij}##, are essential in differential geometry, particularly in the context of smooth manifolds with affine connections. They represent the coefficients of the covariant derivative ##\nabla## in a given chart, allowing for coordinate computations such as calculating the covariant derivative of vector fields. Specifically, they facilitate the transition from Cartesian to curvilinear coordinates by accounting for the changes in coordinate basis vectors with spatial position.

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  • Understanding of smooth manifolds and affine connections
  • Familiarity with coordinate systems and basis vectors
  • Knowledge of covariant derivatives and their applications
  • Basic concepts of differential geometry
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  • Study the properties and applications of affine connections in differential geometry
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Mathematicians, physicists, and students in advanced geometry or general relativity who seek to understand the role of Christoffel symbols in the context of smooth manifolds and their applications in various fields.

dynamic_master
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I'm having trouble understanding what Christoffel symbols are. In simple language, what are they? What are they used for?
 
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Consider a smooth manifold ##M## with affine connection ##\nabla##. Let ##(U,\varphi)## be a chart on ##M## and denote by ##\{\partial_i\}## the coordinate basis associated with this chart. Then the Christoffel symbols ##\Gamma^{k}{}{}_{ij}## associated with ##\{\partial_i\}## are simply given by ##\nabla_{\partial_i}\partial_j = \Gamma^{k}{}{}_{ij}\partial_k##. In other words, they represent the coefficients of ##\nabla## in the chart ##(U,\varphi)## and allow one to do coordinate computations using ##\nabla## such as calculating the covariant derivative ##\nabla_{l}V^{m} = \partial_l V^m + \Gamma^{m}{}{}_{lk}V^{k}##.
 
dynamic_master said:
I'm having trouble understanding what Christoffel symbols are. In simple language, what are they? What are they used for?
Hi dynamic_master. Welcome to physics forums.

If you have a vector quantity (field) expressed in component form and you want to find out how the vector changes with spatial position, then, in cartesian coordinates, you just take the derivatives of the components. However, if you are using curvilinear coordinates, the coordinate basis vectors (or unit vectors) change with spatial position, and you need to take this into account. This is where the christoffel symbols come in. The partial derivatives of the coordinate basis vectors with respect to spatial position can be expressed as a linear summation of the coordinate basis vectors times the christoffel symbols.
 
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