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Single-Particle Electrodynamics - Assassination Science

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A.8.15<br />

Three-velocity of a particle<br />

The non-covariant three-velocity of a classical particle, as seen in some given<br />

lab frame, is denoted v, and is defined as<br />

v ≡ d t z,<br />

(A.55)<br />

where t is the time-coördinate in that frame.<br />

A.8.16<br />

MCLF of a particle<br />

The momentarily comoving Lorentz frame, or MCLF , of a classical particle<br />

at any given instant of time is defined to be the lab frame in which the<br />

particle’s instantaneous three-velocity v vanishes, and its mechanical energy<br />

is greater than zero.<br />

The MCLF is often referred to by the alternative term instantaneous rest<br />

frame.<br />

Note that the MCLF is a Lorentz frame, and remains so for all time. If<br />

the particle is being accelerated, then the MCLF at one moment will not be<br />

the MCLF at the next instant; the latter is a new Lorentz frame.<br />

A.8.17<br />

CACS of a particle<br />

The co-accelerated coördinate system of a classical particle, or CACS, is a<br />

system of coördinates that is co-accelerated with the particle.<br />

Unless the particle is unaccelerated for all time, the CACS does not constitute<br />

a Lorentz frame.<br />

A.8.18<br />

MCLF and CACS components<br />

Components of quantities evaluated in the MCLF (or, in general, any other<br />

Lorentz frame) may be denoted by surrounding the dereferenced quantity by<br />

353

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