Relativistic Frames of Reference

From New IAC Wiki
Jump to navigation Jump to search
\underline{Navigation}

Relativistic Frames of Reference

From the Galilean description of motion for a frame of reference moving relative to another frame considered stationary we know that


Galilean Frames of Reference
Figure 2.1: Primed reference frame moving in the z direction with velocity v.


t=t
x=x
y=y
z=z+vt


Using Einstein's Theory of Relativity, we know that the speed of light is a constant, c, for all reference frames. In the unprimed frame, from the definition of speed:


speed=ΔDistanceΔTime


c=ΔdΔt


where

c=3×108 m/s

Using the distance equation in a Cartesian coordinate system, the equation for the speed of light becomes


c=(Δx)2+(Δy)2+(Δz)2Δt


Following the postulate of Special Relativity, this implies for the primed frame


c=(Δx)2+(Δy)2+(Δz)2Δt



We can rewrite this as


c2=(Δx)2+(Δy)2+(Δz)2(Δt)2     c2=(Δx)2+(Δy)2+(Δz)2(Δt)2


c2Δt2=(Δx)2+(Δy)2+(Δz)2     c2Δt2=(Δx)2+(Δy)2+(Δz)2


\underline{Navigation}