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Riemannian Geometry

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Introduction to General Relativity

Part of the book series: Undergraduate Lecture Notes in Physics ((ULNP))

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Abstract

In the previous chapters, we studied non-gravitational phenomena in inertial reference frames, and often we limited our discussion to Cartesian coordinate systems. Now we want to include gravity, non-inertial reference frames, and general coordinate systems. The aim of this chapter is to introduce some mathematical tools necessary to achieve this goal. We follow quite a heuristic approach. The term Riemannian geometry is used when we deal with a differentiable manifold equipped with a metric tensor.

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Notes

  1. 1.

    A test-particle must have a sufficiently small mass, size, etc. such that its mass does not significantly alter the background gravitational field, tidal forces can be ignored, etc.

Reference

  1. M.H. Protter, C.B. Morrey, A First Course in Real Analysis (Springer, New York, 1991)

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Authors and Affiliations

Authors

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Correspondence to Cosimo Bambi .

Problems

Problems

5.1

Write the components of the following tensors:

$$\begin{aligned} \nabla _\mu A_{\alpha \beta } \, , \quad \nabla _\mu A^{\alpha \beta } \, , \quad \nabla _\mu A^\alpha _{\,\,\beta } \, , \quad \nabla _\mu A_\alpha ^{\,\,\beta } \, , \quad \end{aligned}$$
(5.99)

5.2

Write the non-vanishing components of the Riemann tensor, the Ricci tensor, and the scalar curvature for the Minkowski spacetime in spherical coordinates.

5.3

Check that the Ricci tensor is symmetric.

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Cite this chapter

Bambi, C. (2018). Riemannian Geometry. In: Introduction to General Relativity. Undergraduate Lecture Notes in Physics. Springer, Singapore. https://doi.org/10.1007/978-981-13-1090-4_5

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