stevmg
- 696
- 3
starthaus said:Here is a crash course.
1. Rotation in 2D plane is:
x'=x*cos(\phi)+y*sin(\phi)
y'=-x*sin(\phi)+y*cos(\phi)
You can convince yourself that this is correct by trying to plot a few images.
2. Lorentz transforms :
x'=x*cosh(\phi)-(ct)*sinh(\phi)
(ct)'=-x*sinh(\phi)+(ct)*cosh(\phi)
Because the Lorentz transforms look like the 2D transforms for rotation they are called, by abuse of language, "rotations in the hyperbolic plane". This is where the "rotation" comes from.
It doesn't get any "crashier" than that.
There is some sort of axis rotation, though as shown in this diagram whose thumbnail is shown below. I still don't know how to post a damn picture into the text as others do and I do follow the instructions. It seems that the t' axis is rotated clockwise and the x' axis is rotated counterclockwise towards each other presumably as the v (or \beta) is increased as they squeeze onto the light cone.
But I see your point as the "rotation" was brought about by analogy to the analytical geometry or linear algebra rotating axes.
I assume you have taken chemistry in your studies. If you ever want to see "abusive notation" just take a course in biochemistry where they don't care about equation balance or anything of the like. They are just flow diagrams and not good ones at that (Krebs Cycle, etc.) but that is a different story for another distant distant time.
So rotation of both t and x axes ("squishing") is for Lorentz transforms. Rotation of ONE axis (the t-axis) is for Galilean transformations (no time dilation which causes the "upward" rotation of the x-axis in the "squishing" described above. I presume that is also called "shear" (rotation of t-axis alone.) The clockwise motion of the t'-axis in the moving FR would be caused by the same "shear" as seen in Galilean transformations but not as severe as the gamma factor contracts length and would shorten the angle of clockwise rotation. Click on the thumbnail and you will see more clearly what I am talking about.
"Shear" = Galilean
"Squishing" or stretching (the opposite of "squishing" is Lorentzian.
Of course, if we look at the O' FR by itself, both the t'axis and x'axis are perpendicular and it would be the O FR which would be out of whack (I guess "unsquished" the other way.)
?Right sheet of music?
Attachments
Last edited: