General Relativity For Teletubbies

Sir Kevin Aylward B.Sc., Warden of the Kings Ale


Introduction

This set of papers forms an introduction to General Relativity, in as simple a manner as possible.

The goal of this approach is get to some sort of sensible comprehension of general relativity (G.R.) with out cluttering up the mind with all sorts of extraneous nonsense thatís not required, and only usually given in standard texts to try and impress you on how clever the author is.

To mathematicians this approach will be akin to fingernails on a blackboard, but I'm an EE, and see no need to complicate matters with such posh talk.

Its is assumed that the basic concepts of things such as why the grass is Greens, how to Div funds to offshore banking accounts, and how to Stoke a coal fire on a train has already been covered in other vector analysis courses. Certain things will be systematically ignored because every book by Tom, Dick and Harry already covers it. For example, proving that such and such is really a tensor and that tensor equations are true in all coordinate systems and so forth is a simple waste of time, the goal is to get a good grip on G.R., not pure mathematics. What's much more of use to have step by step derivations that donít jump about into hyperspace leaving you wondering why you seem so thick for not understanding something of real relevance. Usually the author was on drugs at the time and had no concept at all of what a logical argument was.

I have added some background math, just to get those of you punters who are more intellectually challenged up to relativistic speed.


Simplified Summary

1 Its is experimentally observed that all masses, in the same gravitational field, fall with the same acceleration. 

2 Gravitational fields are generated by a mass.

3 There is a geometrical mathematical object, Gab, the contracted Riemann Tensor, that measures acceleration of geodesics (shortest distance between points on a curved surface).

4 There is a physical object, Tab, the energy-momentum tensor, that measures the motion of mass (and energy).

5 Both Gab and Tab satisfy the same mathematical identity, that is Gab;b = Tab;b = 0

6 Therefore if Tab is set equal to Gab, then mass motion will be described by a geometric object that determines acceleration of geodesics, which necessarily means that it satisfies the physical observation of mass generating accelerations if mass moves along a geodesic. 


Contents

Special Relativity

Calculus - basic differential stuff.

Tensors

Covariant Derivative

Calculus of Variations needed to derive the geodesic equation

Geodesic

Riemann Tensor

Stress-Energy/Energy-Momentum Tensor - this is the one that generates the stress of life, we could do well without this.

Einstein Tensor 

Misc. Stuff

E=MC2

If you want to understand what GR is, and what it is not, have a deko at covariance_relativity.pdf. To wit, GR is not Covariance, GR contradicts Mach's Principle, and all accelerating frames are not equivalent.


PDF Versions

sr.pdf
srbackground.pdf
postulate1.pdf
calculus.pdf
tensors.pdf
covariant_derivative.pdf
calculus_of_variations.pdf
geodesic.pdf
riemann.pdf
stress_energy.pdf
einstien_tensor.pdf
emc2.pdf


Links

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