Re: Some Beginner SR Questions



Dean Elliot:
>"Bill Hobba" <bhobba@xxxxxxxxxxxxxx> wrote:
>
>> Consider the origin of the two systems to coincide i.e. if
>> Xu = 0 then X'u = 0. Now suppose Xu = 0 then from the calculus delta X'u
>> A delta Xu for some 4x4 matrix A.
>
>I'm at a loss to understand this matrix. Since you arrive at via calculus
>I assume that it is the result of partial derivatives.

x' = (I + a)x I is the identity matrix, a is an infinitesimal
displacement of each element of x along each direction.

>Could you give a simple concrete example for me? (You can see that if
>things are not explained in detail then I get bogged down trying to
>understand them.)

Check any classical mechanics text book under ``rotations.'' The only
difference between that and relativity is that for 3-d rotations,
g_uv is the identity matrix, diag{1,1,1} and in relativity the
metrix is g_uv = diag{-1,1,1,1}. The relativistic derivation proceeds
exactly the same way. You get 3-d rotations (sine and cosine) plus
spacetime rotations which are hyperbolic sines and cosines due to
the -1. If you understand euclidean rotations, then you'll understand
spacetime rotations.


.



Relevant Pages

  • Re: K calculus OK?
    ... > Ken S. Tucker: ... > Radioactive decay is a counter example to that statement. ... > with the cause (the principle of relativity) than by writing them ... > along side the spatial rotations as spacetime rotations. ...
    (sci.physics.relativity)
  • Re: sinh, cosh Lorentz Xformations: illumination or obfuscation?
    ... But in general relativity you can't ignore the ... the metric tensor is indeed a tensor, we must be careful to define all our ... redundant here) rotations. ... we can consider the identity matrix to be the same object in every system. ...
    (sci.physics)
  • Re: K calculus OK?
    ... > as six, four-dimensional rotations. ... IMO, you need to embody the principle of relativity, ... Since we have a good definition of absolute ...
    (sci.physics.relativity)

Quantcast