# Electric field becomes electromagnetic waves if observer is moving

1. Dec 29, 2007

### Ulysees

At school (a long time ago that is) we were taught:

1. a stationary charge produces a static electric field.

2. a moving charge produces a magnetic field, plus an electric field that is slightly different from the original electric field of the stationary charge.

3. a periodically accelerating charge like an electron in a dipole produces electromagnetic waves. For example, electrons accelerating up and down in a dipole produce waves like these:

What happens if the observer moves, and the charge is stationary? Since it is the relative velocity that matters, the moving observer will experience a magnetic field (plus an electric field, slightly different from the static electric field).

Observers moving at different speeds will experience different magnetic fluxes at the same point in space! So it is not a fixed property of space, the magnetic field is a property of moving charges, different for each observer depending on the velocity of each observer.

But here's another interesting fact about moving observers:

A periodically accelerating observer will experience electromagnetic waves, if stationary charges exist nearby.

In other words, stationary charges emit electromagnetic waves, as far as this observer is concerned!!!

For example an observer is going up and down at each pixel of the following picture, instead of electrons going up and down in the dipole. Also there is no dipole, only a fixed stationary charge in the centre.

Here is a video of the waves experienced by observers at each pixel.

http://web.mit.edu/~sdavies/MacData...7/TuesdayFeb20/graphics/SmPointDipole_640.mpg

So maybe if you go to the magnetic north pole of the earth, and put a campus on the edge of a rotating disk, then at the right rate of rotation the campus will register no magnetic force!

Or maybe not. Maybe I have the maths wrong, magnetic fields do not superimpose linearly, right? Can someone provide the full maths of electromagnetic forces between moving and accelerating point charges please, the full equations for the forces that is, anyone?

If the conclusion is correct, ie that superposition of magnetic fields due to different rotations of the iron in the earth's core is LINEAR, then how fast does the disk have to rotate, in order for the campus to register no magnetic field? (diagram not to scale of course, magnetic field can be assumed constant in the vicinity of the campus and disk).

------------
PS. How do I show the pictures in full size in the post?

Last edited: Dec 29, 2007
2. Dec 29, 2007

### Staff: Mentor

Hi Ulysees, welcome to PF.
This is a good insight. You are exactly correct. The electric and magnetic fields are frame-dependentent quantities that are unified in relativity as the electromagnetic field, just like time and space are unified into spacetime, and energy and momentum are unified into the 4-momentum. You will want to learn about electromagnetism in relativity. If you don't already have a good background in 4-vectors and Minkowski geometry, then you may want to start with those concepts first.

Here are a couple of wiki links to get you started:
http://en.wikipedia.org/wiki/Formulation_of_Maxwell's_equations_in_special_relativity
http://en.wikipedia.org/wiki/Four-vector

Be aware, both the oscillating and rotating frames that you are talking about are non-inertial. So you will have to add all sorts of "correction" terms and ficticious forces in order to use them.

Last edited: Dec 29, 2007
3. Dec 30, 2007

### Ulysees

Thanks for the links and the information.

I was wondering, as a first step in a search for the true meaning of magnetic field which is really what I was after when I drew that rotating observer at the north pole, can you initially assume velocities are well below the speed of light to avoid relativistic equations?

In other words, what are the classical equations for the electromagnetic field of a moving charge?

1. A point charge that moves is not really equivalent to current in electromagnetic equations, is it?

2. If N charges move, can I just add up the magnetic field from each charge to get the total magnetic field? If not, how do I add them up?

3. 1 coulomb moving at 1 m/s is the same "current" as 2 coulombs running at 0.5 m/s, so they produce the same magnetic field B at a given point P, right? But then, at what speed does the observer at P have to move, in order to cancel the magnetic field B, 1 m/s or 0.5 m/s? What if both charges run at the same time? Something is wrong here. Any thoughts?

Last edited: Dec 30, 2007
4. Dec 30, 2007

### Staff: Mentor

I don't know enough about electromagmetism in non-inertial reference frames to answer that question. Basically, in non-inertial coordinate systems you have to introduce "ficticious forces" to make mechanics work. I would assume that you would have to introduce ficticious charges or fields or currents or something similar to get EM to work, but I don't really know.

That said, my gut feeling is that you could not neglect relativistic effects even at low angular velocities. EM forces are so strong that relativistic effects can become important when changing between inertial reference frames even for velocities on the order of 1 m/s.

Start here:

You will see that the Biot-Savart law is simply the superposition of the magnetic field from each of an infinite number of infinitesimal moving point charges in order to get the total magnetic field.

It doesn't matter. Let's say that you have a current in a wire and a moving charge nearby which experiences a certain force due to the magnetic field. If you assume that the current is due to 1 C moving at 1 m/s and transform to the 1 m/s "rest" frame of the current then relativistic length contraction will give you a charge imbalance which will result in an electric field which will give the same force on the charge. If you assume that the current is due to 2 C moving at .5 m/s and transform to the 1 m/s frame then you will have both a magnetic and an electric field, but the net force on the charge will still be the same!

5. Jan 3, 2008

### Troels

If you want som more formal in the matter, I can recommend D. J. Griffiths "Introduction to electro Dynamics" (isbn: 0-13-919960-8) chapter 12 on electrodynamics and relativity

6. Jan 3, 2008

### Ulysees

Thanks everyone.

I guess fictitious forces have to do with being in the frame of reference of a lift that is falling freely, for example, in which frame the earth seems to be accelerating towards the lift at 9.8 m/s^2, therefore a fictitious force F=Mg must be acting on the earth. Likewise to an oscillating observer of stationary charges, they seem to be accelerating, therefore fictional forces must be acting on them. If the observer is oscillating slowly, I guess fictional forces do not matter, it's straightforward Biot-Savart law in its point-charge version, but at relativistic speeds, Biot-Savart is drastically modified, right?

Especially considering the time it takes for the wave to go from the charge to the observer. Or is it the other way round?

Strange that an observer that is oscillating fast enough, will in theory experience radiowaves or even light from a stationary charge! Can this possibly be right?

Last edited: Jan 3, 2008
7. Jan 3, 2008

### Troels

Wel no and yes. The forces do the acceleration on the point charge and thats it. But first of all, there is no "point-charge version" of the Biot-Savart law, though many textbooks state the relation

$$\mathbf{B}=\frac{\mu_0}{4\pi}\frac{q\mathbf{v}\times\mathbf{\hat r}}{r^2}$$

as being such. It is only approxmimately correct for point charges in linear motion, but certainly not if the charge is accelerating and/or moving at relativistic speeds

The fields of a point charge in motion (I thus assume that is it the observer in the rest frame), can be calculated in two ways: relative to the rest frame using the retarded (yes they are called that) Liénard-Wiechert potentials or by calculating the (static) electric field in the moving frame and using the methods of relativistic electrodymanics to transform the fields to the restframe. The latter is usually much simpler.

I will again advise D. J. Griffiths for very beautyfull examples on how both is done

Last edited: Jan 3, 2008
8. Jan 9, 2008

### Ulysees

I have tried to get hold of Griffiths but I have not found the time yet for a visit to a university library. It's available with "Search Inside" in amazon though, any chance you could point me to those beautiful examples you mentioned? (just a a key phrase and a page number would do, from the second method).

Thanks.

Last edited: Jan 9, 2008
9. Jan 10, 2008

### Troels

Well in order to get the full point, I'd say you will need the full last three chapters (i.e chp. 10 Potentials and fields, chp 11 Radiation, chp 12 Electrodynamics and relativity)

That, of course depends on what you already know. If you already are familiar with the time dependent generalization of the electric and magnetic potential, gauge transformations, dipole radiation and basic special relativity, you might settle for sec 10.3, sec 11.2 and sec 12.3

The relativistic transformation of electromagnetic fields are discussed in section 12.3 in the subsections 12.3.2 "how the fields transform" and 12.3.3 "The field tensor" (page 525 through 540 in 3rd ed.)

Last edited: Jan 10, 2008
10. Jan 11, 2008

### Ulysees

Thanks. It will take me some time because I don't know much. But seems a great book indeed, thanks again.

11. Jan 12, 2008

### Troels

I think I will have to restrain myself a bit in the future, because it just occured to me that the transformations of fields in relativistic electrodynamics are treated in the special relativity and thus under the assumption that the moving frame is moving with constant velocity, whereas your particular problem calls for a frame that is accelerating. It is well-known that the special theory of relativity breaks down once you bring acceleration into the equation, so I wouldn't dare bet my head on that the transformations stated in Griffith still hold if you do.

Thus you may be safer off to do it the brute force way, using retarted potentials and classic point charge radiation. The argument of relativity should still apply though, that is, a stationary point charge will appear to be oscilating to an observer in an oscilating frame and will produce radiation accordingly.

Only thing that nags me is how the radiation reaction would fit into al this... The observer would claim that the point charge is damped in its oscilation, because the radiation caries off kinetic energy. But if the charge it stationary, then it would have to be the observer who is damped in his motion! Otherwise, there would be a violation on energy-conservation. Could it be that the charge exert a damping force in on the observer as he detects it's field? Or is there some other mechanism at work? Interresting scheme to say the least...

Last edited: Jan 12, 2008
12. Jan 14, 2008

### Ulysees

In other words, what are the action-reaction force pairs involved here? I guess the charge experiences the reaction, delayed. So action and reaction are not simultaneous, right?

Last edited: Jan 14, 2008
13. Jan 14, 2008

### Ulysees

In the end there is no such thing as field, there is only interaction between charges. Delayed interaction that is.

An observer cannot measure fields without using a device, and inevitably the device is based on forces experienced by charges in it.

Last edited: Jan 14, 2008
14. Jan 15, 2008

### Staff: Mentor

Ficticious forces in non-inertial coordinate systems do not have action-reaction pairs. For instance, there is no reaction force to the centrifugal force in a rotating reference frame. So adding the ficticious centrifugal force helps Newton's 2nd law to work, but causes Newton's 3rd law to fail.

I certainly would not make such a statement. The fields carry momentum and store energy so trying to claim that they do not exist will ruin all of your conservation principles. I don't know what criteria you would use to say that they don't exist.

EDIT: On the other hand, they are frame variant quantities. In that sense they are more like energy or time than mass which is invariant.

Last edited: Jan 15, 2008
15. Jan 15, 2008

### Ulysees

You're right.

I was wondering what the equation is, that gives the momentum of a given field as a function of E and B at a given point and time. Does anyone have it handy?

16. Jan 16, 2008

### dst

Sorry to interrupt but if you could trace the field from an oscillating electron, would it be in the form of rapidly expanding and alternating tori as the first cross section suggests?

17. Jan 16, 2008

### Ulysees

Not necessarily, depends how the electron oscillates, I guess the cross section is exactly as shown for a sinusoidal oscillation, like in a dipole.

-----------

PS. Can someone tell me the policy on diagrams? What's stopping us from showing diagrams in full clear size? Can't I just host them on imageshack.net so they don't consume the forum bandwidth?