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sqljunkey
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Can an everyday magnet disturb a ray of light. I have seen many answers online saying no, and some saying yes, but only if the magnetic field is large enough.
Not in free space, however powerful the magnet. The same applies to crossing beams of light; no interaction.only if the magnetic field is large enough
The magnetic field of an 'everyday magnet' is not energetic enough to produce gravitational effects sufficient to 'disturb' a ray of light
At high enough energies the EM Force can produce 'gravitational effects', including bending light rays, by curving spacetime.Huh??sysprog said:The magnetic field of an 'everyday magnet' is not energetic enough to produce gravitational effects sufficient to 'disturb' a ray of light
Magnetic fields don't produce gravitational fields
Mass does
The rest of that post includes material (e.g. tensor field equations) that I think exceeds 'B' level thread standards.Just looking at general relativity: the answer to the question: "Can a light be bent by a magnetic field?" is yes it can be bent due to the curvature of spacetime produced by a strong magnetic field. I can give a very short answer why, without going into too much detail, how the resulting bent geodesics might look ...
At high enough energies the EM Force can produce 'gravitational effects', including bending light rays, by curving spacetime.
From: a stackexchange post by user M. J. Steil (Sep 5 '16 at 21:02):
The rest of that post includes material (e.g. tensor field equations) that I think exceeds 'B' level thread standards.
However, in some substances, the fields due to an intense beam of light can cause non-linear effects and the fields can affect each other.
You mean the Zeeman effect by that? https://en.wikipedia.org/wiki/Zeeman_effect ,
You mean the Zeeman effect by that? https://en.wikipedia.org/wiki/Zeeman_effect ,
An electromagnetic field curves spacetime by its energy-momentum tensor. This tensor sources gravity in Einsteins theory of general relativity.
An electromagnetic field curves spacetime by its energy-momentum tensor. This tensor sources gravity in Einsteins theory of general relativity.
This effect is, however, very weak.
I think I introduced some confusion when I made reference to 'gravitational effects'. @davenn correctly pointed out that gravitational effects are due to mass. You correctly made reference to EMF spacetime curvature being due to the energy-momentum tensor. At very high energies, this 'very weak' effect is no longer so weak as to be negligible, but at ordinary energies, it is well-established that electromagnetic fields produce no observable bending of light.An electromagnetic field curves spacetime by its energy-momentum tensor. This tensor sources gravity in Einsteins theory of general relativity.
This effect is, however, very weak.
I was under the impression that observations of neutron stars and pulsars had been accounted to evince the EMF contribution to spacetime curvature, i.e. the observed mass doesn't account for all of the observed curvature in their vicinity, but with inclusion of the EMF energy-momentum tensor it does.Instead of describing it as "... very weak.. ", try "...has never been observed before...". This is clearer to the general public, and probably will straighten out the OP who may have read similar statement and thinks that this has been verified.
Zz.
However, in some substances, the fields due to an intense beam of light can cause non-linear effects and the fields can affect each other.
The magnetic field is not even slightly disturbing the light ray itself; it's strongly affecting the material through which the light is passing.sqljunkey said:I get it now. I guess one could argue that since an "everyday magnet" is surrounded by air molecules usually, which is a medium , there would be slight disturbance in the light ray due to the Faraday Effect.
Which in turn disturbs the light yes.The magnetic field is not even slightly disturbing the light ray itself; it's strongly affecting the material through which the light is passing.
In other words, it's affecting the geodesic by which the light follows, yes?it's strongly affecting the material through which the light is passing.
Yes, just as a ferrometallic metal mirror being warped by a magnet could change the path of reflected light, but that wouldn't be EMF bending light -- other than under certain very limited exceptional conditions, EMF cannot bend or otherwise affect light.Which in turn disturbs the light yes.
No. Those are not other words for the same thing. The geodesic in GR is referential to spacetime curvature; not to such things as refractive index or polarization characteristics of semi-transparent materials.In other words, it's affecting the geodesic by which the light follows, yes?sysprog said:it's strongly affecting the material through which the light is passing.
Let me clarify... I was referring to the original question, not anything to do with the Zeeman effect or the Faraday effect. Your quote from the stack exchange post seems to say that the magnetic field affects the geodesic which light follows... is that correct?No. Those are not other words for the same thing. The geodesic in GR is referential to spacetime curvature; not to such things as refractive index or polarization characteristics of semi-transparent materials.
Yes. That's possibly-inferentially-observably true only in very exceptional high-energy conditions. An 'everyday magnet', as in the original question, cannot bend light.Let me clarify... I was referring to the original question, not anything to do with the Zeeman effect or the Faraday effect. Your quote from the stack exchange post seems to say that the magnetic field affects the geodesic which light follows... is that correct?
Not sure. The waves will both have E and H fields so I don't know how you would classify it. (But why bother if it doesn't contribute to the understanding?)You meant Faraday Effect instead of the Zeeman effect?
28–3 Electromagnetic mass
Where does the mass come from? In our laws of mechanics we have supposed that every object “carries” a thing we call the mass—which also means that it “carries” a momentum proportional to its velocity. Now we discover that it is understandable that a charged particle carries a momentum proportional to its velocity. It might, in fact, be that the mass is just the effect of electrodynamics. The origin of mass has until now been unexplained. We have at last in the theory of electrodynamics a grand opportunity to understand something that we never understood before. It comes out of the blue—or rather, from Maxwell and Poynting—that any charged particle will have a momentum proportional to its velocity just from electromagnetic influences.
Let’s be conservative and say, for a moment, that there are two kinds of mass—that the total momentum of an object could be the sum of a mechanical momentum and the electromagnetic momentum. The mechanical momentum is the “mechanical” mass, ##m_{\text{mech}}##, times ##v##. In experiments where we measure the mass of a particle by seeing how much momentum it has, or how it swings around in an orbit, we are measuring the total mass. We say generally that the momentum is the total mass ##(m_{\text{mech}}+m_{\text{elec}})## times the velocity. So the observed mass can consist of two pieces (or possibly more if we include other fields): a mechanical piece plus an electromagnetic piece. We know that there is definitely an electromagnetic piece, and we have a formula for it. And there is the thrilling possibility that the mechanical piece is not there at all—that the mass is all electromagnetic.