The intermolecular rotational potential energies for poly(dimethylsiloxane) (PDMS) chains aredirectly obtained from a priori probability Pαβ. Here the differing statistical weight matrices for the Si-Oand O-Si bonds are considered in calculating the configuration partition function. In the Bahar's model
asthe same statistical weight matrices for the Si -O and O- Si bonds are adopted
there exists a large deviationof α priori probability Pαβ between the theory and the molecular dynamics (MD) simulation. Our model gives satisfactory agreement with experiment on the mean-square unperturbed end-to-end distance
the mean-square dipole moment and its temperature dependence
and the molar cyclization equilibrium constants for dimethylsiloxane oligomers.This new rotational isomeric state approach can be widely applied to other chains
such as —CH2—C[(CH2)mH]2—and —O—Si(CH2)mH]2 for arbitrary m.
Abstract
The intermolecular rotational potential energies for poly(dimethylsiloxane) (PDMS) chains aredirectly obtained from a priori probability Pαβ. Here the differing statistical weight matrices for the Si-Oand O-Si bonds are considered in calculating the configuration partition function. In the Bahar's model
asthe same statistical weight matrices for the Si -O and O- Si bonds are adopted
there exists a large deviationof α priori probability Pαβ between the theory and the molecular dynamics (MD) simulation. Our model gives satisfactory agreement with experiment on the mean-square unperturbed end-to-end distance
the mean-square dipole moment and its temperature dependence
and the molar cyclization equilibrium constants for dimethylsiloxane oligomers.This new rotational isomeric state approach can be widely applied to other chains
such as —CH2—C[(CH2)mH]2—and —O—Si(CH2)mH]2 for arbitrary m.
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