Electromagnetism uniqueness theorem explained
The electromagnetism uniqueness theorem states the uniqueness (but not necessarily the existence) of a solution to Maxwell's equations, if the boundary conditions provided satisfy the following requirements:[1] [2]
- At
, the
initial values of all fields (and) everywhere (in the entire volume considered) is specified;
- For all times (of consideration), the component of either the electric field or the magnetic field tangential to the boundary surface (
or
, where
is the
normal vector at a point on the boundary surface) is specified.
Note that this theorem must not be misunderstood as that providing boundary conditions (or the field solution itself) uniquely fixes a source distribution, when the source distribution is outside of the volume specified in the initial condition. One example is that the field outside a uniformly charged sphere may also be produced by a point charge placed at the center of the sphere instead, i.e. the source needed to produce such field at a boundary outside the sphere is not unique.
See also
References
- Book: L.D. Landau, E.M. Lifshitz . 1975 . The Classical Theory of Fields . 4th . 2 . . 978-0-7506-2768-9.
- Book: J. D. Jackson . 1998 . Classical Electrodynamics . 3rd . . 978-0-471-30932-1.
- Specific
- Book: Smith, Glenn S.. An Introduction to Classical Electromagnetic Radiation. 1997-08-13. Cambridge University Press. 9780521586986. en.
- Web site: 2020-05-11 . 2.8: Uniqueness Theorem . 2022-12-11 . Physics LibreTexts . en.