robinpike said:
That is a good try at trying to solve the problem... but it fails - for it simply replaces the change in the rate of ticks of the clock, with a change in the length of the spacetime path.
The same problem still persists, but now becomes: if the initial acceleration reduces the length of the traveling twin's spacetime path as compared to the stay at home twin's spacetime path, how does the traveling twin use acceleration at the end of his journey to return to the stay at home twin's spacetime path?
(And on a point of understanding your description of a spacetime path, not sure how the shorter spacetime path can return to the stay at home twin's longer space time path? Is the stay at home twin's spacetime path curved or something?)
There are two different aspects to time dilation and the twin paradox: The first is understanding how mutual time dilation (each twin views the other twin's clock to be running slow) can produce an asymmetric result (the traveling twin's clock advances less for the whole trip than the stay-at-home twin). The second is the non-Euclidean metric of Minkowsky space. The first aspect has a direct analogy with Euclidean geometry. The second does not.
By the "non-Euclidean metric of Minkowsky space", I mean this: In Euclidean geometry, if you have a line segment that runs from point A to point B, and the displacement in going from A to B is X in the x-direction and Y in the y-direction, then then length of the line segment L is given by L
2 = X
2 + Y
2. In contrast, if point A and B are points in Minkowsky space, and the separation is X in the x-direction and T in the time-direction, then the proper time of the inertial path connecting A and B is given by L
2 = (cT)
2 - X
2. That minus sign is the reason moving clocks run slower, instead of faster. I don't know of a really good way to understand why spacetime has that minus sign in its metric, other than working with it and seeing how it fits together. For example, if you assume that light has speed c in all directions in one frame, and you assume that getting a straight rod moving in a direction perpendicular to its length doesn't change that length, then you automatically get time dilation for a moving "light clock" formed by a pair of mirrors on either end of a moving rod, with a pulse of light bouncing back and forth between them.
But a lot of the trouble have with the twin paradox is not in accepting time dilation, it's in understanding how
MUTUAL time dilation can lead to an asymmetric result in the elapsed times of the two twins. This is where the analogy with Euclidean geometry helps.
You have two roads that intersect at point A. The "slope" of the second road relative to the first road is m. (Slope is the tangent of the angle between the roads). If s
1 is the distance along the first road, and s
2 is the distance along the second road, then we can relate the two as follows:
Imagine being at a point on the first road at distance marker s
1 , and looking in the perpendicular direction toward the second road to see what the "corresponding" distance marker is there. Euclidean geometry predicts that
ds_2 = ds_1 \sqrt{1+m^2}
So ds_2 > ds_1
If you move ds_1 along the first road, then the corresponding distance marker on the second road changes by a greater amount, ds_2. But this effect is completely mutual! A traveler on the second road comparing the distance marker s_2 to the corresponding distance marker s_1 on the first road (which he sees by looking in a direction perpendicular to his road) will likewise find:
ds_1 = ds_2 \sqrt{1+m^2}
So ds_2 > ds_1
That seems like a contradiction. The first traveler thinks that the markers on the second road are increasing faster, and the second traveler thinks that the markers on the first road are increasing faster. How can they both be right? It's because while each traveler sets up a correspondence between markers on one road and markers on the other road, they use a
DIFFERENT correspondence. The traveler on the first road associates two points on a line perpendicular to the first road, while the traveler on the second road associates two points on a line perpendicular to the second road. Those are two different correspondences.
Now, if the first road continues straight, but the second road makes a turn and comes back to meet the first road, then the first traveler can compute the relationship between distance markers on the two roads as follows:
s_2 at finish = s_2 at start + \Delta s_2
where \Delta s_2 is computed by
\Delta s_2 = \int \sqrt{1+m^2} ds_1
If the slope m is greater than 0 anywhere along the route, then
\Delta s_2 > \Delta s_1
This is the same mystery as in the twin paradox. Slope is
relative, each traveler thinks that the other road has a nonzero slope. But when the two roads get back together, the difference in distance markers along the two roads is objective. How is that possible? Why can't the traveler on the "bent" road use the analogous formula to conclude that \Delta s_1 > \Delta s_2?
The answer is that when the second road makes a turn, its notion of the "perpendicular" direction changes, and its notion of the "corresponding" point on the other road also changes. The formula
ds_2 = ds_1 \sqrt{1+m^2}
doesn't take into account these abrupt changes of the correspondence. From the point of view of the traveler on the "bent" road, the corresponding distance marker on the first road leaps forward or backward suddenly when he makes the turn. This is exactly what happens in the twin paradox to the traveling twin. During turn-around, the traveling twin's notion of how old the stay-at-home twin changes abruptly.