How Do You Transform Electromagnetic Dipole Moments When Boosting Orthogonally?

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SUMMARY

This discussion focuses on transforming electromagnetic dipole moments, specifically magnetic dipole moments (μ), when applying a Lorentz boost orthogonal to μ. The participant explores methods to determine the resulting electric dipole moment in the new frame, considering the linear dependence of magnetic fields on μ and the electric field's relation to the magnetic field. They suggest using the Lagrangian in terms of moments and emphasize the importance of covariant expressions, noting that the electric and magnetic dipole moment densities form an antisymmetric 2nd-rank tensor in Minkowski space-time, which transforms under Lorentz transformations.

PREREQUISITES
  • Understanding of electromagnetic dipole moments
  • Familiarity with Lorentz transformations
  • Knowledge of tensor calculus in Minkowski space-time
  • Experience with Lagrangian mechanics
NEXT STEPS
  • Study the transformation properties of 2nd-rank tensors under Lorentz transformations
  • Research the relationship between electric and magnetic dipole moments in electromagnetic theory
  • Learn about the magnetization-polarization tensor and its applications
  • Explore covariant formulations of electromagnetic fields and their implications
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Physicists, particularly those specializing in electromagnetism and relativistic physics, as well as researchers working on theoretical frameworks involving dipole moments and Lorentz transformations.

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I just wondered how I transform electromagnetic dipole moments.
For example assuming I have magnetic dipole moment μ in a frame without E dipole moment. Then I boost orthogonal to μ. Now I would like to determine the electric dipole moment.

I could use the magnetic potential and transform it to the new frame. But this quiet tedious to me.
My second guess was to argue that there is a linear dependence of the magnetic fields on μ.
And the E field in the new frame will also have a linear dependence on B and thus on μ. By looking at the boost component I could also find a relation. But this would assume that I have an electric dipole moment in the new frame.

I just wondered whether there is any easier and more elegant method.
I would be very glad about any advise.
Thank you :D
 
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Just a thought: writing the Lagrangian in terms of moments.
 
It's just better to start from covariant expressions. As the electromagnetic field itself the electric and magnetic dipole moment densities build an antisymmetric 2nd-rank tensor in Minkowski space-time:

M^{\alpha \beta}=\begin{pmatrix}<br /> 0 &amp; P_1 &amp; P_2 &amp; P_3 \\ <br /> -P_1 &amp; 0 &amp; -M_3 &amp; M_2 \\<br /> -P_2 &amp; M_3 &amp; 0 &amp; -M_1 \\<br /> -P_3 &amp; -M_2 &amp; M_1 &amp; 0<br /> \end{pmatrix},
where \vec{P} and \vec{M} are the electric and magnetic dipole density vector fields of the 1+3-dimensional formalism.

They transform under Lorentz transformations as any other 2nd rank tensor components
M&#039;^{\gamma \delta} = {\Lambda^{\gamma}}_{\alpha} {\Lambda^{\delta}}_{\beta} M^{\alpha \beta}.
 
oh really? I was looking for sth like this. that's good thank you!
 
Magnetization-polarization tensor I found it now
 

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