Axis Alignment in Einstein's 1905 Paper: Symmetry Impact

  • Thread starter Thread starter jason12345
  • Start date Start date
  • Tags Tags
    alignment Axis
jason12345
Messages
108
Reaction score
0
In Einstein's 1905 paper he says that, by reasons of symmetry, we can assume the coordinate axis of the stationary and moving frame are aligned.

If the y and z axis rotate towards/away from the x-axis in the moving frame in a way dependent upon the velocity, how does this break the symmetry of the problem?

Thanks.
 
Physics news on Phys.org
Einstein's stationary and moving frame are both inertial … the axes cannot rotate.
 
If instead you are saying that I have 2 frames which are not aligned (e.g. the x-axis doesn't point where the x'-axis points), what happens? The math gets a lot more complicated, but the physical results stay the same. There's no reason to construct 2 coordinate systems which don't align in SR.
 
jason12345 said:
In Einstein's 1905 paper he says that, by reasons of symmetry, we can assume the coordinate axis of the stationary and moving frame are aligned.

If the y and z axis rotate towards/away from the x-axis in the moving frame in a way dependent upon the velocity, how does this break the symmetry of the problem?

Thanks.

You get a set of transforms that look very similar to Lorentz , see for example :

H. Nikolic,
"Proper co-ordinates of non-inertial observers and rotation",
gr-qc/0307011, invited contribution to the book "Relativity in Rotating Frames", editors G. Rizzi and M. L. Ruggiero, Kluwer Academic Publishers, Dordrecht (2004)
 
tiny-tim said:
Einstein's stationary and moving frame are both inertial … the axes cannot rotate.

I wasn't implying that they rotate continuously with time.

If a set of axis are at right angles in their proper frame, why should they remain at right angles when viewed from a moving frame?

Einstein suggests they must remain so for symmetry reasons and i think i can see why now, partly.

The y and z axis can be flipped with the negative to give another stationary frame with the moving frame traveling along the same x-axis in the same direction. This means the transformation at (x,-y,z) = (x,y,z) and likewise (x, 0+dy, z)= (x, 0-dy, z), for example. So there is no variation of the moving axis y' wrt x and likewise with z'.
 
jason12345 said:
I wasn't implying that they rotate continuously with time.

If a set of axis are at right angles in their proper frame, why should they remain at right angles when viewed from a moving frame?

Then, what you want is this. This is the most general form of the Lorentz transform.
 
Thread 'Can this experiment break Lorentz symmetry?'
1. The Big Idea: According to Einstein’s relativity, all motion is relative. You can’t tell if you’re moving at a constant velocity without looking outside. But what if there is a universal “rest frame” (like the old idea of the “ether”)? This experiment tries to find out by looking for tiny, directional differences in how objects move inside a sealed box. 2. How It Works: The Two-Stage Process Imagine a perfectly isolated spacecraft (our lab) moving through space at some unknown speed V...
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. The Relativator was sold by (as printed) Atomic Laboratories, Inc. 3086 Claremont Ave, Berkeley 5, California , which seems to be a division of Cenco Instruments (Central Scientific Company)... Source: https://www.physicsforums.com/insights/relativator-circular-slide-rule-simulated-with-desmos/ by @robphy
In Philippe G. Ciarlet's book 'An introduction to differential geometry', He gives the integrability conditions of the differential equations like this: $$ \partial_{i} F_{lj}=L^p_{ij} F_{lp},\,\,\,F_{ij}(x_0)=F^0_{ij}. $$ The integrability conditions for the existence of a global solution ##F_{lj}## is: $$ R^i_{jkl}\equiv\partial_k L^i_{jl}-\partial_l L^i_{jk}+L^h_{jl} L^i_{hk}-L^h_{jk} L^i_{hl}=0 $$ Then from the equation: $$\nabla_b e_a= \Gamma^c_{ab} e_c$$ Using cartesian basis ## e_I...
Back
Top