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Single-Particle Electrodynamics - Assassination Science

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mately chosen, both for simplicity, and to ensure a standard result that could<br />

be run on any machine—the author already having been burnt previously<br />

by the implementation-dependencies of C++, which has not, unfortunately,<br />

been standardised as yet.<br />

Of course, the output of computer programs must always be eyed suspiciously,<br />

being only as reliable as the programmer’s concentration level at the<br />

most fatigued point of his work. It is for this reason that the fully checked,<br />

manually-obtained results for the electric charge field contributions to the<br />

radiation reaction terms—computed from beginning to end—were crucial,<br />

for the purpose of debugging the program at each stage of its development.<br />

The computations up to n of the final-order-in-ε results were also important,<br />

in order to verify that the algorithms were correctly handling the extra order<br />

of complexity involved. Once the integrity of the system had been exhaustively<br />

verified, the remaining computations were performing exclusively by<br />

computer—being, of course, too lengthy to continue further on paper.<br />

At a late stage, it was recognised that the definition of the relativistically<br />

rigid body originally used by the author did not correctly handle the subtle<br />

Thomas precession of the constituents, as the body made the transition to<br />

a finite velocity and acceleration (see Section 3.3). This rendered almost<br />

all of the author’s manually-computed results erroneous, in the lower orders.<br />

Fortunately, the program radreact was completed before this oversight was<br />

noted, and it was quite a minor task adding the extra precession expression<br />

to the program.<br />

When the program was then run anew, it was found that, indeed, practically<br />

all expressions which contained sufficient orders in τ or ε (specifically,<br />

those for which terms involving both ˙v and ¨v were present) were changed<br />

by the redefinition of the rigid body. However,—and most surprisingly,—the<br />

final radiation reaction equations of motion were not changed at all, despite<br />

the fact that even the penultimate equations had significant modifications.<br />

Although the deep physical meaning behind such an “invariance” of the re-<br />

414

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