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Single-Particle Electrodynamics - Assassination Science

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G.2 Description of the programs<br />

There are five computer algebra programs, written by the author, that have<br />

been used in the preparation of this thesis: radreact, kinemats, retfield,<br />

test3int and checkrs.<br />

A brief description of each program, and the reasons for its existence,<br />

follow.<br />

G.2.1<br />

radreact: Radiation reaction<br />

When the author first made an attack on the radiation reaction calculations<br />

of Chapter 6, he expanded the Taylor series (2.84) to two fewer orders than<br />

now appear. This was sufficient to compute the electric charge radiation<br />

reaction self-force—i.e., the Lorentz calculation, corrected by the author with<br />

the gravitational redshift factor;—and, while more algebraically complicated<br />

than the naïve Lorentz model of Galilean rigidity, the expressions involved<br />

were not overly onerous.<br />

The successful correction of the Lorentz derivation led to plans of its<br />

extension to the dipole moments. The first stage, of course, was the computation<br />

of the explicit retarded fields from the dipole—now presented in<br />

Chapter 5; this had not, at the time, yet been performed. Once it was<br />

found that they were obtainable in a reasonably simple form, the radiation<br />

reaction calculations were begun. It was immediately clear that, due to the<br />

1/R 3 rather than 1/R 2 variation of the static fields, an extra order would be<br />

required in the calculations. This was begun.<br />

During this task, further comtemplation revealed that the only practical<br />

way of computing the gradient dipole forces—other than the unpalatable<br />

prospect of computing the retarded four-gradients explicitly, and painfully<br />

trying anew to simplify them—was by including yet another order of ε in the<br />

retarded field expressions, and then using the explicit r d and r s (and hence<br />

411

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