The radiation-reaction problem of standard Lorentz electrodynamics with point charges is pathological, standing in contrast to Bopp–Landé–Thomas–Podolsky (BLTP) electrodynamics where it is in fact well-defined and calculable, as reported in a previous publication. To demonstrate the viability of BLTP electrodynamics, we consider the BLTP analogue of the radiation reaction of a classical point charge accelerated from rest by a static homogeneous capacitor plate field, and calculate it up to in a formal expansion about in powers of , Bopp’s reciprocal length, a new electrodynamics parameter introduced by BLTP theory. In a paper by Carley and Kiessling (arXiv:2303.01720 [physics.class-ph]) the radiation-reaction corrections to test-particle motion were explicitly computed to , the first non-vanishing order. In this article a crucial question regarding this ``small-’’ expansion, raised by Carley and Kiessling, is answered as follows: The motions computed with terms included are mathematically accurate approximations to {physically reasonable} solutions of the actual BLTP initial value problem for short times , viz. when , where is the speed of light in vacuo, but their unphysical behavior over {much} longer times does not accurately approximate the actual BLTP solutions even when the dimensionless parameter , where is the elementary charge and the bare rest mass of the electron. This has the important implication that BLTP electrodynamics remains a viable contender for an accurate classical electrodynamics with point charges that does not suffer from the infinite self-interaction problems of textbook Lorentz electrodynamics with point charges.

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