bobc2 said:
ghwellsjr, you have been considering your graphics to represent just one frame of reference.
Yes, that's because in Special Relativity, a given scenario is presented in the context of just one IRF, or if it isn't, calculations are made to eventually get it into a single IRF. Otherwise, it will be ambiguous and impossible to analyze.
bobc2 said:
I'm thinking that your sketch actually implies three sets of coordinates, and you have used the Lorentz transformations to assign values to the time dimensions (X4 = ct) of the other two time coordinates.
I start with the IRF presented by the OP and make a graph corresponding to that IRF. Now in that graph, I calculate the spacing of the dots for each observer, including the stationary one, using the time dilation equation (not the Lorentz Transform). So for each observer/clock, I use the speed assigned by the OP to calculate gamma and gamma times speed. Then I space the dots along the time axis according to gamma and space the dots along the distance axis according to gamma times speed. The Lorentz Transformation is not used to create the data for the original scenario in its IRF, only the Time Dilation factor (gamma) and the speed are used.
You should not think of the blue vertical line with the blue dots as being associated with the time coordinate of the IRF anymore than for the other observer/clock. In another scenario, an OP might not have any observer/clock at rest in the IRF and so there would be no vertical line with dots in the defining IRF.
bobc2 said:
You haven't labled your coordinate time axes, so I've added in the labels for your three time coordinates in sketch a) below.
As K^2 pointed out, there is only one set of coordinates, clearly labeled and marked and providing grid lines so that the coordinates of any event can be easily determined. What you are calling coordinate time axes are not axes at all, they simply show how the Proper Time of each observer/clock advances as a function of the clearly labeled coordinate time
I could have numbered the dots to make it easier to see what time is on each clock but that would have been more work for me so I leave it up to the viewer to count the dots if they care what the Proper Time is at any point in the diagram.
The whole purpose of this exercise is to show that Time Dilation is the ratio of accumulated Coordinate Time to accumulated Proper Time and that it changes with each IRF but still everything comes out the same for anything that the observers/clocks can see, observe and measure.
Since you want to talk only in terms of coordinate time, what is your definition of Time Dilation?
bobc2 said:
Sketch b) just explicitly includes the X1 coordinate axes for the three sets of coordinates used in your presentation. The X1 axes are easy to identify since we know that in any frame the photon of light worldline must bisect the angle between X1 and X4. That assures that the speed of of light will be the same in all frames and the coordinate systems will all be in conformance with Einstein's postulate asserting the laws of physics are the same for all frames. The numbers on the coordinates in your presentation make it clear that you have done a good job of applying the Lorentz transformations between the various sets of coordinate systems.
If you want to see how the speed of light remains c with respect to the IRF even after you transform to a different IRF, I will show you a bunch of graphs illustrating this. Keep in mind once I set up the original scenario, I merely put in a speed parameter to get each of these different graphs. It is the super simple Lorentz Transformation calculation done on all the points (events) of the original graph that creates each new graph. (I do have to do a little more work to limit the scope of each graph to the significant area.) Since I can only upload three graphs in each post, I will continue this in a second post.
First. a repeat of the original scenario with a flash of light sent out by both observers each month according to their own clocks. The thicker yellow lines are sent out by the blue observer and the thinner black lines are sent out by the black observer.
You can note that during the first part of the scenario, each observer sees the other ones clock advancing by the same amount. For example, after 19 months for each observer, they are seeing the other observer at 11 months.
Similarly, during the last part of the scenario, each observer sees the other ones clock advancing by the same (but different than before) amount. For example, between blue's Proper Time going from 41 to 48 months which is 7 months, he sees 12 new flashes coming from the black observer and for the black observer between the coordinates of about 38 and 46, his clock advances by 7 months and he sees 12 new flashes coming from the blue observer.
Now for the next two graphs transformed at 0.5c and -0.5c:
If you care to count out how each observer sees the other ones time progressing just like I described earlier, you can count out the dots to see that it doesn't make any difference what IRF we use, the same information is present in all of them.
Continued on next post...