Optics, electromagnetic theory Maxwell's equations Problem
Abraham–Minkowski controversy
Builds on Maxwell's equationsElectric displacement fieldMagnetic fieldElectric fieldRefractive index
Problem
Let a linear, homogeneous and non-dispersive dielectric medium at rest have permittivity and permeability . Let , be the electric and magnetic field, the electric displacement field and . The problem is to decide which density is the momentum density of the electromagnetic field in the medium: For a light pulse of energy in a medium of refractive index , the two choices give the momenta and .
Remarks
The two densities differ by the factor , so they agree only in vacuum. Both come from energy–momentum tensors of the field in matter that are consistent with Maxwell's equations in the medium; the Minkowski tensor is not symmetric, the Abraham tensor is. The difference is a momentum carried by the medium, so the question is how the total momentum of the light and the medium is split. A widely accepted view is that both answers are correct for different notions. The Abraham momentum is the kinetic momentum of the light, and the Minkowski momentum is its canonical momentum. Experiments measure the total momentum transfer, and different experiments are explained by one or the other expression once the force on the medium is included.
Reading path
To understand this page from the ground up, read these 6 pages in order. The foundations come first.
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- no evidence level
- Electric displacement field concept
- Electric field concept
- Magnetic field concept
- Maxwell's equations concept
- Refractive index concept
- Abraham–Minkowski controversy problem
Further reading
About this page
| Tag | P0CC1763WY |
|---|---|
| URI | m2://P0CC1763WY |
| Kind | problem |
| Writing | W0 stub |
| MSC | 78A25, 78A02 |
| Status | This copy of the site has no build data. Run m2 status P0CC1763WY. |
| About | Electric field, Magnetic field |
| Uses | Maxwell's equations, Electric displacement field, Magnetic field, Electric field, Refractive index |
| Same as | |
| Changed | 3 November 2026 |
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