The second virial coefficient
A2 (
A2(θ
l)) for ring polymers in dilute solution at the theta temperature of the corresponding linear polymers, θ
l, is investigated. It is interesting that the ring polymers at θ
l show a positive value of
A2(θ
l), although the excluded volume of the polymer segments apparently disappears at θ
l. This is a consequence of the topological interaction due to a constraint that the topological state of each of the ring polymers is to be conserved. The value of
A2(θ
l) can be directly derived from the linking probability
Plink, which is defined by the probability that two ring polymers are mutually entangled so that they make a nontrivial link type. Recently, we have numerically evaluated
Plink precisely for random polygons (RPs) with several different values of the step number
N. We have found a good approximate formula for
Plink as a function of
N which should be valid for arbitrary values of
N. Consequently, we obtained a theoretical curve of
A2(θ
l) as a function of
N through this formula. Rather recently, Takano
et. al. obtained extremely pure ring polystyrenes by using liquid chromatography at the critical condition (LCCC) and measured the dependence of
A2(θ
l) on their molecular weight
Mw. In this paper, we compare the theoretical curve of
A2(θ
l)
vs.
N calculated by
Plink with the experimental data of
A2(θ
l)
vs.
Mw. Here we assume that
Mw should be proportional to
N. The qualitative behavior of the theoretical curve is consistent with the experimental data; quantitatively, however, the theoretical values are slightly larger than the experimental values. This result suggests that we should take into account some other effects also in the theory such as the three-body interaction (
A3), as well as the topological interaction.
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