yogi said:
Hyrkyl - I will address a couple of your points which are crucial to your position - you claim that the clocks cannot be compared at the end of the one way trip - yes they can - I have stated that there is a clock on alpha that is in sync with the Earth clock (they are in the same frame and both clocks read proper Earth time and the separation distance is a proper Earth length) - when the traveler arrives the traveling clock will be together with the alpha clock and can be compared. If you state that SR dictates that these two clocks (the one fixed to alpha and the one carried by the traveler) read different times when the traveler arrives then there is no twin paradox because you are defacto advancing LR explanation
No, because in SR there is the Relativity of Simultaneity. Let's by-pass any acceleration for now and just assume that our traveler is making a high speed fly-by of both the Earth and Alpha. We'll assume that the Ship clock can pass so close to the Earth and Alpha clock, so that at that instant the two clocks can be regarded as being at the same point, and that both Any observer can take a instant "snap-shot" of the clocks at this moment of passing to compare their readings.
According to the Earth and Alpha clocks, the Traveler speeds by and crosses the distance in some given time, but due to time dilation, the traveler clock runs slow and thus when it passes Alpha less time will have accumlated on the traveler clock then on either Earth or Alpha.
According to the Traveler the Earth and Alpha fly by in order and it takes a certain amount of time from the instant the Earth passes to the instant Alpha passes. Since the distance between Alpha and Earth undergoes length Contraction, the Time that the Traveler's clock records between the Passing of the Earth and Alpha then the Earth clock records in its Frame for the Traver to pass from Earth to Alpha. In fact the length contraction makes it work out that both the Traveler and the Earth agree as to what time is on the Traveler clock when it passes Alpha (but for different reasons).
The Traveler will also measure time dilation as effecting the Alpha and Earth clocks and will determine that less time will have accumulated on them between their respective passing.
But, According to the Traveler, the Earth and Alpha Clock
are not in sync. They run at the same rate but the Alpha clock will read a more advanced time then the Earth clock. Thus when the Earth passes by and reads a certain time, at that instant the Alpha clock reads a much later time. Adding this Alpha clock reading to the time dilated accumulated time of the Alpha clock will give a certain time on the Alpha Clock it passes the Traveler. And this time will be the same as the time the An Earth observer would read on the Alpha clock as the traveler and Alpha Passed each other.
Again both observers agree as to what time is on both clocks, read when they pass each other,
but for different reasons According to Earth the times read the way they do because the Traver clock ran slow, and according to the Traveler the times read the way they do becuase, While the Alpha clock ran slow, the time it started at( at the instant the Earth and traveler passed) was later than that that the Earth observer determined it was at that instant.
- in LR there is no paradox because the clock that moves relative to the Earth centered reference frame runs slow - no acceleration is needed to distinguish the traveling sibling from the Earth sibling - no observation in other frames is significant and your own statement from a previous post attempting to explain the triplet paradox by saying that the reading of the outbound sibling's clock by the third inbound sibling will result in an informational change to a different reference frame causing a temporal shift... are exemplary of relatitivsts shifting positions when faced with the reality that clocks in relative motion run at different local rates.
There is no paradox in SR because, when applied fully and correctly all observers will agree as to what time are read on clocks that are local to each other at any given time no matter which observer is considered the stationary one.