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Fig. 7 Definition of coarse grained repeat units (symbolized by circles ) for the 1,4 polybutadiene
chain. The atomistic model is an united atom model of a random copolymer of 45% cis and 55%
trans content, without vinyl units. Bond lengths are constrained
53 A for the CH 2 CH 2 bond,
ð'
1
:
5 A for the CH 2 CH bond and
34 A for the CH CH bond). From Strauch et al. [ 117 ]
'
1
:
'
1
:
coarse-grained (cg) effective monomers i , j . The intramolecular potentials U bond ð
L
Þ
and U angle ð
can be found by the “Boltzmann inversion” [ 105 110 ] from the
probability distribution P
cos
of these degrees of freedom sampled from a
simulation of the full atomistic model. For this simulation of the full atomistic
model, a relatively short run of a relatively small system might suffice, at least in
favorable cases. Thus [ 117 ]:
ð
L
Þ , P
ð
cos
U bond ð
L
Þ¼
k B Tln
½
P
ð
L
Þ;
(12)
U angle ð
cos
YÞ¼
k B Tln
½
P
ð
cos
YÞ:
(13)
Figure 8 shows the resulting potentials at three temperatures. In principle,
effective potentials obtained from the Boltzmann inversion [( 12 ) and ( 13 )] will
contain entropic contributions and, hence, in general must be state-point dependent;
however, Fig. 8 suggests that in favorable cases this dependence is small.
However, it is difficult to obtain the nonbonded interaction from the same route:
in addition, atomistic potentials for nonbonded interactions are often rather unreli-
able. Thus, the form of the nonbonded interaction was chosen to be a priori fixed to
be of the LJ type:
U c LJ ð
n
m
r
Þ¼
4 e pp
ðs pp =
r
Þ
ðs pp =
r
Þ
(14)
 
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