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3 - Differential geometry I: vectors, differential forms and absolute differentiation

Published online by Cambridge University Press:  05 June 2012

Lewis Ryder
Affiliation:
University of Kent, Canterbury
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Summary

It is almost impossible for me to read contemporary mathematicians who, instead of saying, ‘Petya washed his hands’, write ‘There is a t1 < 0 such that the image of t1 under the natural mapping t1 → Petya(t1) belongs to the set of dirty hands, and a t2, t1 < t2 ≤ 0, such that the image of t2 under the above-mentioned mappings belongs to the complement of the set defined in the preceding sentence …

V. I. Arnol'd

In this chapter we introduce the mathematical language which is used to express the theory of General Relativity. A student coming to this subject for the first time has to become acquainted with this language, which is initially something of a challenge. Einstein himself had to learn it (from his friend Marcel Grossmann). The subject is widely known as tensor calculus; it is concerned with tensors and how to define and differentiate them in curved spaces. In more recent times tensor calculus has been recast using a more sophisticated formalism, based on coordinate-free notation and differential forms. At first physicists were disinclined to learn this higher grade language, since it involved more work, without, perhaps, any reward in terms of mathematical or physical insight. Eventually, however, sceptical minds became convinced that there were indeed pay-offs in learning this new formalism, and knowledge of it is now almost essential to read research papers in the field of General Relativity.

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Publisher: Cambridge University Press
Print publication year: 2009

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