In mathematics and physics, the **Christoffel symbols**, named for Elwin Bruno Christoffel (1829–1900), are numerical arrays of real numbers that describe, in coordinates, the effects of parallel transport in curved surfaces and, more generally, manifolds. As such, they are coordinate-space expressions for the Levi-Civita connection derived from the metric tensor. In a broader sense, the connection coefficients of an arbitrary (not necessarily metric) affine connection in a coordinate basis are also called Christoffel symbols. The Christoffel symbols may be used for performing practical calculations in differential geometry. For example, the Riemann curvature tensor can be expressed entirely in terms of the Christoffel symbols and their first partial derivatives.

At each point of the underlying *n*-dimensional manifold, for any local coordinate system, the Christoffel symbol is an array with three dimensions: *n* × *n* × *n*. Each of the *n*3 components is a real number.

Under *linear* coordinate transformations on the manifold, it behaves like a tensor, but under general coordinate transformations, it does not. In many practical problems, most components of the Christoffel symbols are equal to zero, provided the coordinate system and the metric tensor possess some common symmetries.

In general relativity, the Christoffel symbol plays the role of the **gravitational force field** with the corresponding *gravitational potential* being the *metric tensor*.

Read more about Christoffel Symbols: Preliminaries, Definition, Relationship To Index-free Notation, Covariant Derivatives of Tensors, Change of Variable, Applications To General Relativity

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### Famous quotes containing the word symbols:

“As usual I finish the day before the sea, sumptuous this evening beneath the moon, which writes Arab *symbols* with phosphorescent streaks on the slow swells. There is no end to the sky and the waters. How well they accompany sadness!”

—Albert Camus (1913–1960)