and may be presented at high values of R in the power form n(RR Y with the exponent y increasing with R

4.6.3. Non-relativistic case; A and u are functions of R

In this case, according to Eq. 4.6.4, in the non-relativistic range we obtain at

Substituting Eq. 4.6.3 in Eq. 4.4.18 and considering Eq. 4.6.5 we shall find the following equation determining the variations in the particle rigidity R with time t of particle acceleration:

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