Scientists use the Tokyo Skytree to test general relativity
phys.org
phys.org
Gravity in a multi body system or in special cases of a two body system, has counteracting forces. If you found the Lagrange point between a binary black hole system, you could stay there. Or if you hollowed out the core of the Earth, you would float because you are being pulled in all directions at once (essentially the 2 body problem doesn’t “behave” for concave objects or distance less than diameter).
Is time slower or faster at the Earth’s core? Is it slower or faster at the Lagrange point of a three body system?
There is no gravitational acceleration to measure. It's zero.
In the absence of other forces, a body in a gravitational field experiences a constant acceleration that only depends on the strength of the field. In the accelerating reference frame of the object, there are no net forces. You could for example measure the gravitational acceleration of earth by jumping from a plane and measuring how fast the ground is coming towards you.
Time dilation of a clock does not depend on the clock being able to reference some external object, like the earth. (I do recognize you can not measure time dilation until you compare to some other clock.)
So, let's reframe with a thought experiment and maybe you can answer:
A clock in the center of the earth, and a clock dropped from a tall tower on earth (ignore the rotation of the earth). Each clock sends two laser pules, exactly 1/100 of a second apart toward the other clock.
(The falling clock sends its pulses moments after being dropped, so it has essentially zero speed relative to the clock in the center of the earth.)
The partner clock then measures how far apart in time it received the two pules.
After that we collect the reports from the clocks and evaluate.
Will the two clocks each report the same time interval?
For an even better experiment lets add a third clock, this one resting on the surface of the earth.
Einstein used a free-falling sealed box to derive the equivalence principle. This does not imply that any free-falling system is a sealed box. Thinking about clocks makes absolutely no sense without having a way of comparing them.
In your example, the clock in the center of the earth will run slower than the one falling from the tower due to gravitational time dilation. Note that Einstein's "light clock" thought experiments do not capture this effect, since it stems from General Relativity, not Special Relativity.
That is a more complicated question than is immediately apparent because it is not just the curvature of spacetime that is in play, it is also the fact that objects that are supported at the surface of the earth are effectively being accelerated upwards (through spacetime) by that support. An object at the center of the earth doesn't need any support to remain in place, so it is in an inertial frame. To really do an apples-to-apples comparison of the effect of spacetime curvature alone you'd need one clock at the center of the earth and another in orbit so that each clock would be in a locally inertial frame. But now you have special relativistic effects because the two clocks are in relative motion. So there is no absolute answer to the question. It depends on which frame of reference you use. The clock in orbit will think the one at the center of the earth is slow, the one at the center will think the clock in orbit is slow (this is essentially the classic twin paradox).
A clock at the center of the Earth runs more slowly than a clock on Earth's surface.
The answer to your Lagrange point question is probably indeterminate. The differences in clock rates depend on the relative depths in potential not the magnitude of gravitational force (as measured by anyone).
Viewed another way, the hill beside our lab deflects the direction of "down" by about 50 nanoradians for every meter you move vertically in the lab. (If you kept the hill, and got rid of the earth, a satellite would orbit the hill.)
The really crazy thing about the experiments described in the article is that they depend on the difference in potential, which is much harder to estimate. As these clock-based experiments reach still-higher sensitivities, we're going to see improved and interesting tests of gravity emerge alongside the increasingly-difficult problems of time-transfer at these levels of precision.
(We care about this difference-in-the-direction-of-down because we need to lock one of our turntables to "local vertical" with nanoradian stability. It was initially a surprise, before my time, when it was realized that it was impossible to do so simultaneously for two sensors on the same turntable but at different locations on the turntable axis.)
Also, if you think that's cool, depending on your latitude, the "down" you experience doesn't point in the direction of the center of the earth. The earth is rotating, so there is a substantial centrifugal contribution to the acceleration you experience. Off the top of my head, I believe the effect here in Seattle is about 14 milliradians. It is zero at the pole and equator (the apparent centrifugal acceleration makes you effectively lighter!), though :).
Holy moly. Just what kind of measurements are you doing in your lab?
Our most-recent measurement: https://news.ycombinator.com/item?id=22797729
Once you know how, it's not as hard as you'd expect to measure a nanoradian ;).
Gravity is, by most measures, our oldest force, and while GR is a very successful theory, we know essentially nothing about the underlying mechanism. This is very much unlike the rest of the Standard Model, where we have very-successful quantum theories.
https://www.hartenergy.com/exclusives/gravity-and-magnetic-g...
https://en.wikipedia.org/wiki/Schiehallion_experiment
"The Royal Society formed the Committee of Attraction to consider the matter, appointing Maskelyne, Joseph Banks and Benjamin Franklin amongst its members"
What they are testing is their ultraprecise clocks, not the theory of general relativity like the headline says.
The Skytree experiment is directly measuring gravitational time dilation which is a central prediction of General Relativity. Combined with an accurate measurement of the height difference and local gravitational acceleration, this makes it a very accurate test of GR.