By Leonor Godinho, José Natário

ISBN-10: 3319086650

ISBN-13: 9783319086651

Unlike many different texts on differential geometry, this textbook additionally deals attention-grabbing purposes to geometric mechanics and common relativity.

The first half is a concise and self-contained creation to the fundamentals of manifolds, differential types, metrics and curvature. the second one half experiences functions to mechanics and relativity together with the proofs of the Hawking and Penrose singularity theorems. it may be independently used for one-semester classes in both of those subjects.

The major rules are illustrated and extra built through a number of examples and over three hundred workouts. special ideas are supplied for plenty of of those workouts, making *An creation to Riemannian Geometry* excellent for self-study.

**Read or Download An Introduction to Riemannian Geometry: With Applications to Mechanics and Relativity PDF**

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**Extra resources for An Introduction to Riemannian Geometry: With Applications to Mechanics and Relativity**

**Example text**

The same is true for any subgroup . For each we can define the orbit of p as the set . If then is called a fixed point of . ), then the action is said to be transitive . Note that when this happens, there is only one orbit and, for every with , there is always an element of the group such that . The manifold is then called a homogeneous space of . The stabilizer (or isotropy subgroup ) of a point is the group The action is called free if all the stabilizers are trivial. If is a Lie group and is a smooth manifold, we say that the action is smooth if the map is differentiable.

1 Let be a coordinate neighborhood on (that is, for some parameterization ), and let be the corresponding coordinate chart. Then a map is a differentiable vector field on if and only if, for some differentiable functions . Proof Let us consider the coordinate chart . As , we have for some functions . e. if and only if the functions are differentiable. 11(1)]. This function is called the directional derivative of along . Thus one can view as a linear operator . Let us now take two vector fields .

Hence does not depend on the choice of , as long as . Moreover, the components of in the basis associated to are where is an matrix (the Jacobian matrix of the local representation of at ). Therefore, is the linear transformation which, on the basis associated to the parameterizations and , is represented by this matrix. 7 The derivative is sometimes called differential of at . Several other notations are often used for , as for example , and . 8 Let be a parameterization around a point . We can view as a differentiable map between two smooth manifolds and we can compute its derivative at For , the th component of is (where is the identity matrix).

### An Introduction to Riemannian Geometry: With Applications to Mechanics and Relativity by Leonor Godinho, José Natário

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