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Why did you stop in the middle? Keep going.Chenkel said:I tried to get equation 3 from 1 and 2
Why did you stop in the middle? Keep going.Chenkel said:I tried to get equation 3 from 1 and 2
I'll try againPeterDonis said:Why did you stop in the middle? Keep going.
Chenkel said:I tried to get equation 3 from 1 and 2:
##x' = \gamma (x - vt)##
##x = \gamma (x' + vt')##
##x = \gamma ( \gamma (x - vt) + vt')##
##\frac x \gamma = \gamma (x - vt) + vt'##
##vt' = \frac x \gamma - \gamma (x - vt)##
Something tells me I might be on the wrong track with my equations but I told you I would try to solve the problem you proposed to me.
I'm trying to understand the symmetry argument to obtain ##x=\gamma(x'+vt')##Sagittarius A-Star said:Solve the shown equation for ##x'##:
- From the light clock scenario, derive time dilation factor ##1/\gamma## and calculate ##\gamma=\frac{1}{\sqrt{1-v^2/c^2}}## with the Pythagorean theorem.
- Use this result and the standard twin paradox scenario to argue, that the length contraction factor must be ##1/\gamma##.
- Derive the Lorentz transformation from length contraction by using the following diagram.
$$x'=\gamma(x-vt) \ \ \ \ \ \ \ \ \ \ (1)$$With a symmetry argument, you get the inverse transformation:
$$x=\gamma(x'+vt')\ \ \ \ \ \ \ \ \ \ (2)$$Eliminate ##x'## between the two previous equations and then solve for ##t'## to get the time transformation:
$$t'=\gamma(t-\frac{v}{c^2}x)\ \ \ \ \ \ \ \ \ \ (3)$$With a symmetry argument, you get the inverse transformation:
$$t=\gamma(t'+\frac{v}{c^2}x')\ \ \ \ \ \ \ \ \ \ (4)$$
Effective learning is possible by not only reading, but if you also solve problems by yourself.
It is good, that you started using LaTeX for writing formulas in posting #1 of this thread.
I propose, that you try to derive step-by-step the above equation (3) from equations (1) and (2) while using ##\gamma=\frac{1}{\sqrt{1-v^2/c^2}}##.
If the primed frame is moving v with respect to the unprimed frame, then the unprimed frame is moving -v with respect to the primed frame. If all inertial frames are equivalent, the transform from prime to unprimed must the the same as the other way, with -v as v.Chenkel said:I'm trying to understand the symmetry argument to obtain ##x=\gamma(x'+vt')##
See the very good explanation of @PAllen in posting #65.Chenkel said:I'm trying to understand the symmetry argument to obtain ##x=\gamma(x'+vt')##
I noticed in the first picture the origin of the primed frame is vt relative to the unprimed frame, this made some sense to me.Sagittarius A-Star said:See the very good explanation of @PAllen in posting #65.
For a visualization, I modified the scenario from posting #59. Now, a red rod is at rest with respect to the "moving" frame ##S## (and length-contracted with respect to frame ##S'##).
If you solve the shown equation for ##x##, then you get the equation you ask for.
Chenkel said:Why would you use the unprimed time over the primed time or the primed time over the unprimed time?
It depends on, which frame I defined as reference frame. See answer above.Chenkel said:If a primed frame is in relative motion to an unprimed frame do you use the primed time to describe the motion or the unprimed time?
You use the quantities from the frame you chose to use. Typically, you will start with the frame where you and your clocks and rulers are at rest and transform to a frame where somebody else is at rest in order to deduce that other person's measurements.Chenkel said:If a primed frame is in relative motion to an unprimed frame do you use the primed time to describe the motion or the unprimed time?
If a primed frame is in relative motion to an unprimed frame, then the unprimed frame is also in relative motion to the primed frame. It's symmetrical, so there is no way to pick the frame "to use" based on that alone.Chenkel said:If a primed frame is in relative motion to an unprimed frame do you use the primed time to describe the motion or the unprimed time?
Chenkel said:If a primed frame is in relative motion to an unprimed frame do you use the primed time to describe the motion or the unprimed time?
Many questions and confusions in special relativityrobphy said:I suggest first looking at the Euclidean analogue: https://en.wikipedia.org/wiki/Rotation_matrix
The entire point of creating the primed and unprimed frames is that they are in relative motion. You use both of them! Otherwise there would be no reason to create both of them.Chenkel said:If a primed frame is in relative motion to an unprimed frame do you use the primed time to describe the motion or the unprimed time?
Chenkel said:The full Lorentz transform I find a little confusing, I don't fully understand the part where ##\frac {v} {c^2} \Delta x'## the units seem to check out but I'm not sure how that quantity is associated with time.
Chenkel said:...
##vt' = \gamma v ({t - x\frac {v}{c^2}})##
##t' = \gamma ({t - \frac {v}{c^2}}x)##
I appreciate that you helped me get that result hopefully I see the big picture and things start making sense.Sagittarius A-Star said:It's the term for "relativity of simultaneity". Such a term appeared also in your calculation: