Macro said:
You lost the argument. :!)
What does acceleration do to the clock?
Acceleration doesn't do anything per se, it's more a geometric issue--if you have two points in spacetime and you draw two worldlines between them, one straight and the other bent (ie a worldline of an object whose velocity was not constant), you will always find that the bent worldline has a shorter proper time (time as measured by a clock that travels along that worldline) than the straight one. This is analogous to the fact that if you draw two points on a piece of paper, then a straight line between the points will always have a shorter length than a bent one.
Technically, if you know the velocity as a function of time v(t) of a clock in a given inertial reference frame, then to find the total time elapsed on the clock between two times in the frame's coordinate system t_0 and t_1, you do the integral \int_{t_0}^{t_1} \sqrt{1 - v(t)^2/c^2} \, dt (because at any given moment, if the clock's velocity at that moment is v then it must be ticking at \sqrt{1 - v^2/c^2} the normal rate in that frame, so you just integrate this to get the total time elapsed on the clock). You will find that if you evaluate this integral for two clocks that depart each other and reunite, it is always true that the result is longer for the clock that had a constant v(t) then the one that had a changing v(t), which is just another way of saying that the clock that accelerates will have elapsed less time.
Macro said:
What are accelerating frames but ones where time and space are
changing.
Special relativity only says that the laws of physics work the same in all
inertial frames, not in accelerating frames (for example, in accelerating frames it's possible for objects to be moving faster than c). Any textbook on SR will tell you this, and Einstein restricted the two postulates of SR to non-accelerating frames in his original 1905 paper.
Macro said:
Only one Twins clock goes slow. Its called the Transverse Doppler Effect and
I say it is soley due to motion through space.
Mitch Raemsch
You're wrong, and you are misunderstanding the most basic idea of what "relativity" is all about. It is easy to see by using the Lorentz transform (which tells you how to translate between different frame's coordinate systems) that the slowdown effect is perfectly symmetrical, and that each observer will say that the other observer's clock is the one that slows down. It might help you to look at an example I provided on the thread
an illustration of relativity with rulers and clocks, showing how if you have two rulers sliding alongside each other at constant velocity with clocks placed at regular intervals along each one, in each ruler's frame it will be the other ruler's clocks that are running slow, and yet this does not lead to any inconsistencies in what the different frames predict about what two clocks read at the moment they pass each other. The specific numbers I used for the ruler-markings and clock times in that example were taken from the Lorentz transform.
I have no idea why you think the transverse doppler effect would contradict this symmetry--as explained http://www.kineticbooks.com/physics/trialpse/41_Special%20Relativity/21/sp.html , the transverse doppler effect has to do with what an observer sees using light-signals when an object is moving along a straight line that does not cross his own position. As long as both the observer and the object are moving inertially, their view of each other will also be symmetrical--we can do a numerical example of this if you like. Also, note that what an observer
sees using light-signals is different from what he says is "really" going on in his own frame--for example, if you're coming towards me I will see your clock running fast due to the doppler effect, even though your clock is really running slow in my frame (the time-coordinates between successive ticks of your clock are longer than normal in my coordinate system, but since you're moving towards me each successive tick happens at a closer distance to me, so the light from each tick takes less time to reach me than the last one and thus your clock appears sped-up when I look through my telescope at you approaching).