I have made this simple. There is a clock at k in the context of the primed frame with k < 0.
The question is from the time the origins are the same to the time k and the unprimed origin is the same, what will be the time on the clock at k and what will be the time on the unprimed origin clock.
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I assume you understand when the origins are the same, t'=t=0.
Next, from the view of the primed frame, the unprimed origin is a distance k from the clock at the unprimed origin when the two origins are the same.
So, the following events are simultaneous in the primed frame:
E1: (x',t')=(0,0); (x,t)=(0,0)
E2: (x',t')=(k,0)
For now, I omit the (x,t) coordinates of event E2, since you can't understand those.
Hopefully, you can understand, the clock at k will elapse -k/v for the unprimed origin to reach k.
In the primed frame, the unprimed origin travels at speed -v, so it takes the time you say in the primed frame: -k/v.
The end event is therefore:
E3: (x',t')=(k,-k/v)
The time interval between events E2 and E3 is -k/v in the primed frame. Similarly, the time interval between events E1 and E3 is -k/v in the primed frame.
The time interval between events E1 and E3 is DIFFERENT than the time interval between events E2 and E3 in the unprimed frame, even though these intervals are the same in the primed frame.
Next, the final question is what is the elapsed time on the unprimed origin clock?
That depends on whether you want the elapsed time between events E1 and E3 or between E2 and E3.
1) From the view of the primed frame, this is standard time dilation so, the primed frame concludes the unprimed origin clock elapses -k/(γv)
In that case, you have calculated the time interval between events E1 and E3 in the unprimed frame. In that case, this is proper time interval in the unprimed frame, but it is not a proper time interval in the primed frame.
Since the proper time interval is expected to be shorter than the other time interval, we expect the time interval to be shorter in the unprimed frame. It is, so this is in accordance with special relativity.
2) From the view of the unprimed frame, since the clock at k is measured in primed frame coordinates, then when the origins are the same, the unprimed frame concludes primed clock at k is a distance k/γ from the unprimed origin.
This is one place you go wrong, since you now introduce event E2: (x',t')=(k,0), which says the clock is at x'=k in the primed frame at time t'=0.
Using the Lorentz transform on that event, we obtain:
E1: (x,t) = (γk,γkv/c^2).
So, when the origins are the same in the primed frame, the primed clock is at distance γk from the unprimed origin, and not k/γ as you claim. However, this does NOT occur at the time that the origins are the same in the unprimed frame.
Since the distance is k/γ to the unprimed origin and the speed is v, then the elapsed time from the view of the unprimed origin on the unprimed origin clock is -k/(γv).
The elapsed time depends on the start and the stop time in the unprimed frame. The start and end events in the unprimed frame are:
E1: (x,t)=(0,0)
E3: (x,t)=(0,-k/γv)
The time interval you have calculated is correct for this pair of events, even if your reasoning is wrong.
Note how both frames agree on the time of the unprimed origin clock. There is no disagreement.
For events E1 and E3 the time intervals are:
$$\Delta t' = -k/v, \Delta t = -k/\gamma v$$
There is, as you say, no disagreement for that pair of events.
So far, we have both frame agree the unprimed origin clock will elapse -k/(γv) from the time the origins are the same to the time the clock at k meets the unprimed origin.
We have the primed frame claiming the clock at k will elapse -k/v.
Last, we need the conclusion of the unprimed frame for the clock at k. This is standard LT. k us measured in light seconds and v is measured in terms of c.
t = -k/(γv)
x = 0
t' = ( t - vx/c² )γ =( -k/(γv) - 0)γ = -k/v.
Let's makes sure we have the correct x'.
x' = ( x - vt )γ = ( 0 - v(-k/(γv))γ = k. Yes, we have the correct x'.
Therefore, both frames agree the clock at k will elapse -k/v.
Both frames agree the clock at the unprimed origin will elapse -k/(γv).
I note that all you have done here is apply the Lorentz transform to event E3, and you have done that correctly for that event.
Finally, we take the view of the unprimed origin and the moving clock at k coming toward the origin beats time expanded as agreed on both frames. And frame agreement is necessary because of the invertibility of LT.
We agree that the time interval between events E1 and E3 is longer in the primed frame than in the unprimed frame.
When you talk about the "moving clock" you are making an assumption about which clock is moving. Between events E1 and E3, the relevant clock is moving according to the primed frame, but stationary according to the unprimed frame. We can see this by observing that the x' coordinate of that clock changes between the two events, while the x coordinate remains the same. So, for these two events, it is best to regard the clock as "moving" in the primed frame.
To repeat: the primed frame watches the clock moving from x'=0 to x'=k. The unprimed frame has a stationary clock that remains at x=0 at all times.
Special relativity says that stationary clocks measure the proper time, so the proper time in this case is measured in the unprimed frame. Special relativity also states that the proper time should be shorter than the time in any other frame. This is true for this particular pair of events.
So, once again we conclude that there is no problem for special relativity here - only problems with chinglu's understanding of special relativity.
To summarize your error, you consider a clock in the unprimed frame at the same location as k when the origins were the same and placed some time on it.
No. That would be to consider event E2. As you can see quite clearly from the current post, I have used the interval you specified: the one between events E1 and E3.
You, on the other hand, seem to have trouble distinguishing between events E1 and E2. You flip-flop from discussing one to discussing the other, without taking any care to make sure you know which one you're talking about at any given time.
That clock at that location is not in any way involved in this problem and has no affect on the conclusions.
Then you should not introduce it into the problem.
Are you now happy that when we use only events E1 and E3 we get the correct answers, in accordance with what special relativity predicts? Yes or no?
We are only concerned with two clocks, the clock at the unprimed origin and the clock at k in the primed frame.
More specifically, we are only concerned with two events: E1 and E3, and we're concerned with the time interval between those two events as measured in both the primed and unprimed frames. We must be careful that if we're comparing time intervals we are always comparing the time interval between the same pair of events.
I end by repeating my challenges to chinglu, since they are still unanswered:
1. Do you agree that if a frame records a proper time interval between two events, then any other frame will record a longer time interval between the same pair of events? Yes or no?
2. Go through any or all of posts #117, #118, #165 or #177 line-by-line, saying clearly whether you agree or disagree with each step and explaining clearly any errors you can find in those posts.
My bet: chinglu will do anything to avoid answering these challenges, especially number 2. So far, this is 100% confirmed.