Little Franklin said:
Thanks.What circumstances would this happen under?
Where is a good place to learn about space-time diagrams?
A space-time diagram is just a graph of position vs time. Usually, though, one makes the time axis vertical in a space-time diagram. This doesn't actually matter, though, it's just the way the graph is usually drawn.
You'll see several examples of space-time diagrams in the FAQ, and in the wikipedia entries.
http://en.wikipedia.org/w/index.php?title=Minkowski_diagram&oldid=136675389
the relativity of simultaneity entry in the wikipedia is also useful and has some space-time diagrams
http://en.wikipedia.org/w/index.php?title=Relativity_of_simultaneity&oldid=138735828
With the clock experiment I sugested, I understand light emited by an object in a greater space-time curve (not sure what the correct decription is) should be red shifted. Couldn't you then measure the relative passage of time by comparing the red/blue shift of the light from the different objects?
I'm not sure what you mean, but I'll describe one way to measure time dilation, which I think is what you're ultimately after.
What you do is this. You, as the lab observer, want to measure time dilation on a moving clock. What you do is set up a huge array of clocks, one every mile. You then carefully synchronize all these clocks. This synchronization operation is frame dependent - i.e. the moving observer will have a different notion of how to synchronize the clocks.
Now, what you do to measure time dilation is that whenever the moving observer passes over the exact same position as one of your huge array of clocks, you compare them on his moving clock with one of your lab clocks while they are exactly at the same point in space. This is how one can measure "when" a distant event occurs. One uses a clock at the location of the distant event, and synchronizes it to some master clock.
The synchronization process is a key element to make this procedure work. Did I mention it was frame dependent? (I think I did, but I want to stress that point!).
Doing this, you will find that the clock on the moving observer always reads lower than his lab clock does.
This is time dilation.
The moving observer can perform an identical experiment and will get the same result - he will find that what we have been calling the "lab clock" always runs slow.
The key to reconcilling these results is the fact that notion of synchronizing the clocks depends on the observer, i.e. the lab-frame clock synchronization is different than the moving frame synchronization.
One quick off topic question, is the path of light of higher wavelengths curved more by gravity than that of lower wavelengths, and if so is the effect the same as that of refraction through water/glass?
Nope. There is no frequency dependence in gravitational lensing.