Peter Martin said:
Thanks for the response. But wasn't Einstein's deflection empirically derived from the photographic plates taken during the eclipse?
Derived, no. Detected, yes. Einstein derived his theory before the deflection experiments were done. The deflection experiments were consistent with Einstein's theory, and showed more deflection of light than "Newtonian theory" would predict. The initial tests were not terribly precise, and some argue that they might not, in retrospect, have been definitive. Later much more precise tests have been done, and these later tests are all consistent with EInstein's theory and not consistent with "Newton's theory". I am not aware of any serious claims that the modern results aren't definitive in ruling out Newtonian gravity.
Exactly what is meant by the Newtonian prediction of the deflection of light may be mildly unclear. I'd suggest looking up the
<<wiki references>> in the following quote to see what the literature had to say about the Newtonian prediction.
wiki said:
Henry Cavendish in 1784 (in an unpublished manuscript) and
Johann Georg von Soldner in 1801 (published in 1804) had pointed out that Newtonian gravity predicts that starlight will bend around a massive object.
For a bit of theoretical background on the 2:1 prediction for light deflection, and on experimental tests of General Relativity, including but not limited to the light deflection tests, I'd suggest reading WIll's "The Confrontation between General Relativity and Experiment",
<<link>>
The following excerpt in particular might be helpful in understanding the significance of the equivalence principle, which is also mentioned by the OP to which this post is a reply. The point I'm trying to make is this. The equivalence principle that the OP cites is called the "weak equivalence principle". There is a stronger version, the "Einstein Equivalence principe", discussed by Wills, which can be thought of as the weak equivalence principle, plus local lorentz invaraince, plus local position invaraince, as the article describes.
Here is the full excerpt:
One elementary equivalence principle is the kind Newton had in mind when he stated that the property of a body called “mass” is proportional to the “weight”, and is known as the weak equivalence principle (WEP). An alternative statement of WEP is that the trajectory of a freely falling body (one not acted upon by such forces as electromagnetism and too small to be affected by tidal gravitational forces) is independent of its internal structure and composition. In the simplest case of dropping two different bodies in a gravitational field, WEP states that the bodies fall with the same acceleration (this is often termed the Universality of Free Fall, or UFF).
A more powerful and far-reaching equivalence principle is known as the Einstein equivalence principle (EEP). It states that:
- WEP is valid.
- The outcome of any local non-gravitational experiment is independent of the velocity of the freely-falling reference frame in which it is performed.
- The outcome of any local non-gravitational experiment is independent of where and when in the universe it is performed.
The second piece of EEP is called local Lorentz invariance (LLI), and the third piece is called local position invariance (LPI).
I am concerned that an important point of this, the feature of Einstein's equivalence principle called "Local Lorentz invariance", nubmer 2 in the list, may not be clear to the original poster or other non-specialist readers. This feature of General Relativity is an outgrowth of Einstein's previous theory, special relativity. Special relativity has also been well tested, one can find some discussions and references of the tests in the relativity forum's FAQ if one feel the need. I will assume that there is no need and that a fuller discussion of tests of SR would be off-topic. The point I'm trying to make is that Einstein's theoretical framework arose from his desire to make gravity consistent with special relativity, and that the technical language to describe this requirement is "local Lorentz invaraince". Furthermore I want to say that Local Lorentz invariance is a key feature of special relativity. The 2:1 deflection was a mathematical result of Einstein's theory, based on these starting assumptions, and the motivation for this was to make gravity fit into the frameork of special relativity. The prediction of light deflection came after the theory was developed as a way to test the theory. Finally, after Einstein made these predictions, the tests were carried out, and confirmed the theory - or more precisely, the tests were consistent with Einstein's theory, and not consistent with Newton's theory (as described by Soldner).
There are other theories than Einstein's theory, generally more complex ones with additional parameters, that also satisfy Einstein's equivalence principle. Experimental work to test General Relativity is typically done in a framework in which it is assumed that one has a metric theory of gravity, which will satisfy EInstein's equivalence principle. See Will's article for more detail on "metric theories of gravity", and this issue in general.