San José State University |
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Fields in 3D Space |
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It was shown in a previous study that Maxwell's equations imply that electromagnetic fields in the absence of charges obey the wave equation
where C is the speed of light in the medium in which the field exists.
In spherical coordinates (r, θ, φ) the Laplacian ∇² is given by
For a spherically symmetric field E in which all the derivatives with respect to the angle coordinates are zero the wave equation reduces to
Now consider the equation
When this is expanded it is
And, when this equation is multiplied by r the result is
The equation
is a one dimensional wave equation in rE. The d'Alembert solution therefore applies; i.e.,
In this solution one half of the field shoots away toward the horizon at the speed of light. The other half moves through the center of the field at the speed of light. It would seem that this other solution is not physically relevant. The physically relevant solution is then
Consider a field generated by a spherical charge of radius R.
If the charge were to disappear the hole in the field would expand from a radius of R at t=0 at the speed of light, as depicted below.
Free fields not generated by a charged particle disappear toward the horizon at the speed of light. There can be no static free-fields. The goal of Quantum Field Theory of replacing charged particles with autonomous free fields is thus grossly misguided.
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