gonegahgah said:
Someone on here a little while ago helped me to understand that instead of the 'trough' that you describe that you actually end up with something called a saddle ridge.
That is that the two planets in the example that we are between have their low points shifted towards each other (hence why they move towards each other) but the low points don't combine to create a common trough. Instead a ridge remains between the two low points.
The balance point is the highest point on a transect connecting the centres of the two planets (in the rubber sheet model) but this point is still not as high as points inifinitely far away. In fact if you start at the saddle point at move on a line that is at right angles to the connecting line, you continue to go uphill to a higher (less negative) potential.
gonegahgah said:
But I have another question in relation to that.
I assume you would measure our relative potential as being our height relative to the height of the planets in the overall space-time topology. So that actually makes our potential less than that of the planets.
Your potential is actually
greater than that of the planets (but less than the potential at infinity). Potential refers to the potential (possibility) of recovering energy by falling. If you fall your potential energy is converted to kinetic energy which is your falling velocity and when you hit the ground the kinetic energy is converted to sound energy and heat energy in a very rough Newtonian sense.
gonegahgah said:
So for us at our point in-between the planets does that mean our clocks due to GR should actually be traveling faster?
Yes, but it would probably be better to say the clocks are ticking faster than the clocks on the planets (but not as fast as a clock at infinity).
We have been banging on about potential in this thread, as that is probably the easiest to way to visualise things (but bear in mind that the rubber sheet model is a crude analogy) and because the Newtonian term for gravitational potential GM/r appears in the gravitation time dilation factor:
\sqrt{1-\frac{2GM}{rc^2}}
However as Ich as hinted at, that is not the whole story.
It is interesting to note that the Newtonian expression for escape velocity is:
v_e = \sqrt{\frac{2GM}{r}}
and when this expression is inserted into the factor above it, the gravitational time dilation factor becomes:
\sqrt{1-\frac{v_{e}^2}{c^2}}
which has a very obvious analogy with time dilation in Special Relativity.
Could it be that escape velocity is the essential ingredient for determining the time dilation at a given point?
All we have to do now, is figure out what the escape velocity on the rim of a rotating wheel is.
turin said:
Can you describe how you would calculate this? I figure that the amount of work depends on how you move the clock. The clock has some initial kinetic energy due to its circular motion, I'll call it KE. Then, I suppose that we place the clock at the center with zero KE. So, the work done on the clock is W = -KE? I must be missing something. Maybe I'm not allowed to stop the rotation first? Does the Coriolis effect come into play?
This relates closely to my comments above about the escape velocity. One definition of escape velocity is the velocity a particle requires for its KE to be equal to the gravitational potential energy at its location. Escape velocity is also equal to the terminal velocity of a particle that falls from infinity to a given height. I imagine this "escape velocity" as it applies to a wheel is the velocity a test weight achieves when it slides frictionlessly along a spoke from the centre of the wheel to the rim of the wheel.