The field equation from Newton's law of motion and the absence of magnetic monopole (Q2716688)
From MaRDI portal
 | This is the item page for this Wikibase entity, intended for internal use and editing purposes. Please use this page instead for the normal view: The field equation from Newton's law of motion and the absence of magnetic monopole |
scientific article; zbMATH DE number 1599323
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | The field equation from Newton's law of motion and the absence of magnetic monopole |
scientific article; zbMATH DE number 1599323 |
Statements
6 January 2002
0 references
self-adjointness
0 references
second order differential operator
0 references
inverse problem
0 references
field equqtions
0 references
electrodynamics
0 references
universal chiral relation
0 references
electric and magnetic monopoles
0 references
0 references
0.8571969
0 references
0.84684926
0 references
0.8361874
0 references
0.83360636
0 references
0.8293225
0 references
0.8288868
0 references
0.82800925
0 references
0 references
The field equation from Newton's law of motion and the absence of magnetic monopole (English)
0 references
First, the authors recall the problem of self-adjointness of the second order differential operator and the inverse problem in classical mechanics. Then, by requiring the linear differential operator in Newton's law of motion to be self-adjoint, the authors obtain the field equations of classical electrodynamics. A fundamental universal chiral relation between electric and magnetic monopoles is established.
0 references
