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RELATIVITY E van Zyl Part III This is the transformation which is needed to convert a reading x'
in the K' system of coordinates to an x value in the K system, if K' moves
with a speed of v relative to the K system. According to classical Galileian / Newtonian
mechanics: x' = x - vt. A light signal along the positive x axis ( to the right )
of frame K is transformed according to the Relative to K' the transformation is x' - ct' = 0 (2) Space-time points ( called events ) which satisfy (1) must also satisfy (2).
i.e.
In the negative direction Add (4) to (3)
i.e.
Equation (3) Equation (4) Subtract (4) from (3)
So
that
i.e.
..So
that The problem now is to find the values of a and b.
For the origin of K', x' = 0
and
v is the relative velocity of the two systems of co-ordinates. The Principle of Relativity states: Relative to K the length of a unit measuring rod at rest to K', must be exactly the same as the length of the rod relative to K' of a unit measuring rod at rest to K. Insert a particular value of t ( time of K ), e.g. t = 0, Then (5 i) becomes x' = ax - bc(0), So that x' = ax If x' increases by 1 unit ( infinitesimally small ) ax = 1 so that Relative to K' where t' = 0 , eliminating t from equations (5 i) and (5 ii) we get: bct = ax - x' and act = ct' + bx . Thus
But
ie
so
that Thus points on the x-axis separated by distance 1 relative to K will be represented by the distance x' = a ( 1 - v2 / c2 )1 and this must be equal to
Equations (6) and (8)
determine the values of a and b . Insert these values of
The time t' can be derived from: It equals the classical transformation divided by |
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