Deriving Bending of Light from Maxwell's Equations

RedX
Messages
963
Reaction score
3
Can the bending of light because of gravity be derived from the Maxwell equations written in curved space time, i.e.,

\frac{1}{\sqrt{-g}}\partial_\mu(\sqrt{-g}F^{\mu\nu}})=0

In all the examples the bending of light is treated as a massless particle traveling on a light-like geodesic (if I understand the examples correctly) with no reference to the electromagnetic field at all.
 
Physics news on Phys.org
Yes, it is possible to show that if light is assumed to be plane waves, then paths that are normal to the planes are null geodesics.

The plane wave ansatz is implemented by setting
F^{\mu\nu}=g^{\rho\mu}g^{\sigma\nu}(A_{\rho,\sigma}-A_{\sigma,\rho})
with
A_\mu=\hat{A}_\mu e^{i\omega S}

The rest of the derivation is rather long. See 'geometrical optics'.
 
I don't know if this has been done directly.

I think usually one shows there is a ray approximation to a solution of the Einstein-Maxwell equations, and these are null geodesics, and then lives with that.

http://arxiv.org/abs/astro-ph/0108255
http://relativity.livingreviews.org/Articles/lrr-2004-9/
 
Last edited by a moderator:
So if you have a massless particle, say a graviton, which is a 2nd-ranked tensor, or a neutrino which is a spinor, then would the bending be exactly the same as for light which is a vector? I would add scalar particles but I'm unaware of any that are massless.

So somehow the mass=0 free solutions of the Dirac, the Maxwell, and spin-2 (is there a name for the spin 2 equation?) equations all have the same solutions?

Also, a quick question on gravitons. It seems to me that the graviton is a very special spin-2 particle. All spin 1/2 particles obey the same equation, the Dirac equation. All spin 0 particles obey the Klein-Gordan equation. But the action for the graviton g_{\mu\nu} is:

S=\int d^4x\sqrt{-g}R

where R=R(g_{\mu \nu}) is the scalar curvature which is a function of the graviton field.

For a generic spin 2 field z_{\mu\nu} that is not the graviton, the action is:

S=\int d^4x \sqrt{-g}R

where R has the same form as the scalar curvature, but the g_{\mu\nu}'s are replaced with z_{\mu\nu}'s.

So it seems the EOM for the graviton and other spin 2 particles are different. Is this right?
 
Last edited:
Well, the classical graviton is a gravitational wave which should travel on null geodesics of the background spacetime.

For other spin 2 particles, I might try searching for bimetric theories http://relativity.livingreviews.org/Articles/lrr-2005-5/ . Lubos Motl had interesting comments on whether it was possible to have another massless spin 2 particle http://motls.blogspot.com/2008/07/bimetric-pseudoscience.html (as you probably know, ignore the rhetoric about "pseudoscience", he usually has good physics comments).
 
Last edited by a moderator:
Thread 'Can this experiment break Lorentz symmetry?'
1. The Big Idea: According to Einstein’s relativity, all motion is relative. You can’t tell if you’re moving at a constant velocity without looking outside. But what if there is a universal “rest frame” (like the old idea of the “ether”)? This experiment tries to find out by looking for tiny, directional differences in how objects move inside a sealed box. 2. How It Works: The Two-Stage Process Imagine a perfectly isolated spacecraft (our lab) moving through space at some unknown speed V...
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. The Relativator was sold by (as printed) Atomic Laboratories, Inc. 3086 Claremont Ave, Berkeley 5, California , which seems to be a division of Cenco Instruments (Central Scientific Company)... Source: https://www.physicsforums.com/insights/relativator-circular-slide-rule-simulated-with-desmos/ by @robphy
Does the speed of light change in a gravitational field depending on whether the direction of travel is parallel to the field, or perpendicular to the field? And is it the same in both directions at each orientation? This question could be answered experimentally to some degree of accuracy. Experiment design: Place two identical clocks A and B on the circumference of a wheel at opposite ends of the diameter of length L. The wheel is positioned upright, i.e., perpendicular to the ground...
Back
Top