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Single-Particle Electrodynamics - Assassination Science

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to us will be on the order of the time required for light to cross the stationary<br />

body—which, in naturalised units, is just 2ε. (From the arguments of<br />

Section 6.1, it is clear that times greater than this static light-distance are<br />

relevant, but they are all larger by a dimensionless factor: they are still of<br />

order ε.) The spatial distances of relevance to us are also, clearly, of order ε.<br />

Thus, in distinction to the analysis of Chapter 3, where we merely expressed<br />

the system’s trajectory in terms of a Taylor series in time for convenience,<br />

for the current application we may expand our expressions out both<br />

temporally and spatially in the small parameter ε—and, more importantly,<br />

we can extract exact self-interaction results, in the point limit ε → 0, since<br />

any terms of order ε or higher in these final expressions will vanish rigorously<br />

in this limit.<br />

6.3.2 Electromagnetic moment densities<br />

There arises the question, in any use of a spherical body in the regularisation<br />

of a point particle, of how one is to distribute the electromagnetic moments<br />

throughout the interior of the volume. The external fields are, for any sensible<br />

choice of distribution, unconcerned about how the sources are arranged (for<br />

the case of the electric charge, this is most simply recognised by considering<br />

Gauss’s law); but the computed mechanical self-field quantities are of course<br />

modified, since they have contributions from the fields both internal and<br />

external to the sphere, which are the same order of magnitude (see, e.g.,<br />

Section 5.5 of Chapter 5).<br />

For the case of simply an electric charge, a spherical charge shell is often<br />

employed (i.e., a sheet of charge around the surface of the sphere). With such<br />

a choice, the charge density is still infinite on the surface, but this infinity is<br />

now one-dimensional, rather than three-dimensional as with a point charge.<br />

This reduction in pathology is, in fact, sufficient for one to analyse the system<br />

without infinities entering the expressions of relevance. It also has the added<br />

233

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