On Wednesday, December 11, 2024 at 2:41:02 PM UTC-7 Jesse Mazer wrote:

On Wed, Dec 11, 2024 at 2:44 AM Alan Grayson <[email protected]> wrote:



On Tuesday, December 10, 2024 at 11:40:10 PM UTC-7 Alan Grayson wrote:

On Tuesday, December 10, 2024 at 11:15:16 PM UTC-7 Brent Meeker wrote:

Do I not only have provide a diagram I also have to explain it in detail 
just to end this silly thread??


*Yes you do. Providing plots without the numerical values in the LT, is 
useless. I can't tell if you're drawing plots to satisfy your biases, or if 
the numbers support the case you're making. Lesson learned; always do a 
real proof, which means supplying the arguments, or STFU. AG *


*Brent; your numbers check out. The car fits with ease from the pov of the 
garage frame, but not from the pov of the car frame. But this bothers me 
since we know that all frames are equivalent in SR. How then can two, 
so-called equivalent frames, gives different results?*


They both give the same results about all local events, like if there were 
clocks mounted to the front and back of the car synchronized in the car 
frame, and clocks mounted to the front and back of the garage synchronized 
in the garage frame, in Brent's example both would agree that when the back 
of the car passed next to the front of the garage, both the clocks mounted 
to car and garage there read 0, and when the front of the car passed the 
back of the garage, the clock mounted to the front of the car read -7.5 and 
the clock mounted to the back of the garage read 3.5. This agreement about 
local events is something I highlighted in my illustration of systems of 
rulers and clocks in relative motion at 
https://physics.stackexchange.com/a/155016/59406 (Einstein used the notion 
of such a system to define the physical meaning of inertial reference 
frames).

Also, when physicists talk about all frames being equivalent, what they are 
usually talking about is the equations expressing the general dynamical 
laws of physics such as Maxwell's equations for electromagnetism, which 
don't depend on the specific arrangement of matter/energy you choose for 
your initial conditions; you can translate these dynamical equations from 
one frame to another via the Lorentz transformation just like you can with 
specific events, and when you do so you find that the equations have 
exactly the same form when expressed in a different inertial coordinate 
system.


*Yes, I am aware of that, e.g., the E and B fields in EM are frame 
dependent, but ME are invariant under the LT. AG*
 

The equations for length contraction and time dilation could be thought of 
as a special case of such general dynamical equations, in that values like 
velocity and rest length are left as variables, so you can plug any 
specific value in depending on the initial conditions you're looking at.

Jesse


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