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R 1
r *
R 2
R 3
a
r
DISTANCE FROM CENTER
Fig. 3.15 Same as in Fig. 3.13 . The energy is positive, E > 0. The ions with L<L.r / reach the
particle surface
Now the energy E 0 .E/ depends on E
R 2
j U.R/ j r 2
j U.r / j
E 0 .E/ D
R 2
r 2
C
3.6.1.3
Repulsion
Singular Attraction
An example is the Coulomb repulsion C image potential (always attractive).
Figure 3.15 explains what is happening. In this case the ions can reach the particle
 
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