This paper continues the study of the Lorentz-Dirac equation taux''' - x" =
d/dx V(x), which aas begun in [6]. In particular, we study the qualitative
behaviour of Dirac's so-called 'non runaway" solutions modelling motions o
f particles which are reftected respectively transmitted by an obstacle giv
en by the potential function V(x). We show that if the potential has a suff
iciently sharp maximum, then the solutions oscillate a certain number of ti
mes around the maximum of the potential before being reflected or transmitt
ed.