yogi said:
Jesse - There is definitely an objective sense to the fact that Q is ageing less at every point in his orbit - we monitor satellite clocks continuously from different ground stations and if the Height is factored out, an uncorrected GPS satellite clock will continually fall behind the ground observer clock - Are you really saying that, relative to the North Pole clock J, Q will be seen it leading and then lagging and that an opposite result would occur at the South Pole...
No, I'm not saying that. Relative to the north pole clock J, Q is always moving at exactly 20,000 miles per hour, so it is always slowed down by the same amount. But relative to the clock K, which is moving inertially at 15,000 mph relative to J (I messed up the numbers in my example last time, if K only saw J moving at 5,000 mph like I said earlier, then K would always see Q moving faster than J), Q's speed varies from between 5,000 mph at the North Pole and 35,000 mph at the South Pole. So at the North Pole K sees Q moving at 5,000 mph to the right and J moving at 15,000 mph to the left, therefore in K's frame at this moment, J's clock is ticking slower than Q's. Do you disagree with this? Do you disagree that K's inertial frame is just as valid for working out the problem as J's inertial frame?
yogi said:
AS to the fact that the Earth is not an inertial system - it is true
I never said that the Earth was not an inertial system, over short time intervals it's acceptable to say that the center of the Earth (and the poles) are moving inertially. I just said that
Q is not an inertial system.
yogi said:
but the experiment can always be adjusted to eliminate the slight curvature when making measurments - For example, in the traveling clock example, B can actually straighten out his curve at any number of destinations (if the curvature bothers you so much) where he wants to take note of the clocks in A frame
That won't help your argument at all, because the point is that in looking at the
entire trip from start to finish, you still can't treat B as if he's in an inertial frame and thus sees A's clock ticking slower throughout the trip. If you analyze the entire problem from within a
single inertial frame, at best B can only be at rest in this frame during
one of the line segments that make up his trip.
yogi said:
so long as his velocity remains at v, the observations of B will indicate that clocks at every point in the A frame are running show
Only if you switch inertial frames in the middle of the problem, but that will involve complexities like B's surface of simultaneity suddenly swinging around, and at those moments A's clock may not be running slow, but instead leaping forward very quickly into the future. You
can't just assume that the normal formulas of relativity like time dilation apply to the perspective of an observer who does not move inertially throughout his trip, like B.
So again, it's better to analyze the entire problem from start to finish from within a single inertial frame. Then you really can say that at any moment, the rate a clock is ticking is determined
solely by its velocity in that frame. And once again, there are perfectly valid inertial frames where B's velocity is slower than A's at certain points in the circle it makes, or where Q's velocity is slower than J's at certain points in its orbit.
yogi said:
And yes - one inertial frame is presumed to be as good as another - but that is where you are missing my point - the individual components of the interval are not the same
I don't know what you mean by "the individual components of the interval".
yogi said:
and that is why, when relativly moving observers only have one piece of data, namely relative velocity, they will both conclude the other clock is running slow (but this is impossible - its an observational fallacy).
Do you also think it's "impossible" that two observers in Newtonian mechanics could each see the other observer's velocity as greater than their own, from the perspective of their respective rest frames? If not, I don't see why two observers who each see the other's clock running slower is any more problematic.
yogi said:
But when there is more data (as Einstein gives you in his physical description in part 4 - namely a rest frame in which both clocks are synced
As long as the clocks start out at the same location, they are synced in
all frames.
yogi said:
and in which real (proper) distances are measured, the spacetime interval for the traveling clock has a spatial component that is a proper distance measured in the original frame where both clocks were initially at rest.
You are making nonsense of the term "proper distance". Einstein would never have said a path can have a proper length, and neither would any other relativist. Go on, ask some others on this board if you don't believe me.
yogi said:
But not vice versa (there is no spatial component in the interval of the stay at home clock) - and that is why age differences are real and permanent, and Albert has told you so.
And so has Yogi
Complete nonsense. Einstein would have said it would be just as valid (though less simple mathematically) to analyze the problem from the perspective of a different inertial frame where A is in motion at constant velocity and B's velocity varies as he moves away from A, and if you analyze the problem in this frame you will get
exactly the same answer for how far B will have fallen behind A when they reunite, (1/2)t(v/c)^2.
That is why the age difference is real, because you will get exactly the same answer for the age difference when they reunite regardless of what frame you use.
Do you agree that we would get the same answer for the age difference when A and B reunite if we used a different frame, and that Einstein and all relativists would say that it would be just as valid to analyze the problem from some other frame besides A's rest frame? Please answer this question yes or no.