Dispersion and Dichroism in Gravitational Fields

In summary, the author is doubtful that the equations derived by Landau and Lifschitz in a GTR-correct form produce the same wavefronts as classical Maxwell's equations in a vacuum. They state that this is a result of an inappropriate approximation, and suggest looking at a specific example in monochromatic electromagnetic plane waves.
  • #1
Satie
6
0
Hi!
Following Landau&Lifschitz (L&L) (I´m not a researcher in GTR) it is possible to arrive to a 3D version of Maxwell equations in a GTR-correct form. These equations resembling the ones in a dispersive electric and magnetic material, suggest, at first glance, that there should be a dispersion relation for EM waves propagating in a gravitational field. In fact, after a naïve algebra-struggling, it is possible to get to equations with a dispersion-like form.
However, if this was true, the radiation of an explosive event would arrive at different times for different wavelenghts, in a classical GTR formulation which is not correct (as far as I know) since then there should be local effects that could tell an observer about absolute positions and velocities with respect to the source.
I know there is some Loop Quantum Gravity results that suggest it is possible, but in Quantum Gravity scenarios, to have this effect.
The point is that I cannot find the L&L-inspired formulation wrong, nor can I accept it.
Can somebody shed some light on this ignorant-fellow?:confused:
 
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  • #2
Can you state which section (in "Classical Theory of Fields", I presume?) you are looking at?

If you think you have found a dispersion relation for EM waves propagating in a vacuum in gtr, you must have goofed (unless I misunderstand what you have in mind). However, this sounds like the kind of mistake which could result from making an inappropriate approximation.

See http://en.wikipedia.org/w/index.php?title=Monochromatic_electromagnetic_plane_wave&oldid=41212306 for a detailed discussion of the simple exact solution (given in closed form) which models, in gtr, an EM plane wave propagating through "empty space"; this wave has a specific frequency and it is a solution to the fully nonlinear field equation. Strangely enough, parallel plane waves are not hard to superimpose (despite the nonlinearity of the EFE), so you should be able to modify this so that you can see two frequency components, and then you will see that the wavefronts move in lockstep: no dispersion.
 
  • #3
Hi! And Thanks! The Section of L&L I am referring to is the Problem Part of Section 90 of The Classical Theory of Fields L&L. They derive the EM field equations in 3D form, using "gamma" determinant and "g" vector. They state that equations 4, 5 and 6 are the 3D versions and they notice the analogy ("purely formal") with Maxwell´s Eq in material bodies. Probably, my mistake was to push this analogy forward and try to eliminate H to get the E equation (just to have a glance to how would it look like). In an isochronous system (vector "g"=0) they are wave equations but with a term proportional to the time-derivative of the field E. If g is not equal zero, there are terms proportional to the curl of E. In the first, the derivative indicates dispersion and in the second dichroism. Of course I am not saying that this is correct.
I know that this cannot be. But all the same, since in Quantum gravity analysis there is some evidence (I am not the one that can tell if this is right ot wrong) that both effects are possible, then I asked where the whole reasoning leads to such unreasonable result in the classical field.
I did not pretend to find flaws in the GTR, nor to have found a "new effect", mine is just plain doubt about the use of such form of Maxwell´s eq...
Thanks again for your next comment! Truly yours
By the way, an e-mail of yours came yesterday but somehow I cannot find it in the server today, so I cannot answer that... sorry!
 

1. What is the Maxwellian puzzle or paradox?

The Maxwellian puzzle or paradox is a thought experiment proposed by James Clerk Maxwell, a renowned physicist, in the 19th century. It involves imagining a hypothetical being with the ability to control and observe the movement of individual atoms, and the paradox arises when this being tries to measure the speed and position of an individual particle at the same time, which according to the Heisenberg uncertainty principle is not possible.

2. What is the significance of the Maxwellian puzzle?

The Maxwellian puzzle highlights the fundamental principles of quantum mechanics, specifically the Heisenberg uncertainty principle. It also challenges our understanding of classical physics, as it shows that the laws that govern the macroscopic world do not necessarily apply at the atomic level.

3. How does the Maxwellian puzzle relate to other paradoxes in physics?

The Maxwellian puzzle is similar to other paradoxes such as Schrödinger's cat and the double-slit experiment, as it highlights the strange and counterintuitive nature of quantum mechanics. However, it is unique in that it focuses on the impossibility of simultaneously measuring certain properties of a particle, rather than the nature of the particle itself.

4. Has the Maxwellian puzzle been solved?

No, the Maxwellian puzzle has not been solved. It is still a subject of debate and discussion among scientists, and it remains an important thought experiment in understanding the principles of quantum mechanics. Some propose that the paradox can be resolved by considering the limitations of our measurement tools, while others argue that it points to the need for a new theory that can reconcile quantum mechanics with classical physics.

5. What are the implications of the Maxwellian puzzle?

The Maxwellian puzzle has significant implications for our understanding of the physical world. It challenges our intuition and common-sense notions of how objects behave, and it highlights the limitations of our current scientific theories. It also has practical implications for technologies such as quantum computing, as it shows the importance of understanding and controlling individual particles at the atomic level.

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