## Molecular basis of polymer networks: proceedings of the 5th IFF-Ill Workshop, Jülich, Fed. Rep. of Germany, October 5-7, 1988The contributors to this volume appraise our knowledge of the molecular physics of polymer networks and pinpoint areas of research where significant advances can be made using new theories and techniques. They describe both theoretical approaches, based on new theoretical concepts and original network models, and recent experimental investigations using SANS, 2H NMR or QELS. These new techniques provide precise information about network behaviour at the molecular level. Reported results of the application of these and more traditional techniques include the microscopic conformation and properties of permanent networks or gels formed by specific interchain interactions, the behaviour of elastomer liquid crystals, and the static and dynamic properties of star-branched polymers. |

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Page 35

Rep. of Germany 2Department of Physics, University of Leeds, Leeds LS29JT,

UK We propose a deformation dependence of the Flory-Huggins interaction

parameter for deformed polymer

...

Rep. of Germany 2Department of Physics, University of Leeds, Leeds LS29JT,

UK We propose a deformation dependence of the Flory-Huggins interaction

parameter for deformed polymer

**blends**, which has its origin In the concentration...

Page 39

Polymeric Fractal

Postfach 3148, D-6500 Mainz, Fed. Rep. of Germany We consider first chemically

identical fractals of different connectivity. This leads to swelling effects of

polymeric ...

Polymeric Fractal

**Blends**TA. Vilgis Max-Planck-Institut fur Polymerforschung,Postfach 3148, D-6500 Mainz, Fed. Rep. of Germany We consider first chemically

identical fractals of different connectivity. This leads to swelling effects of

polymeric ...

Page 45

After some transformations it takes the more simple form -d c f -p = e fJdu *j 5 (18)

0 {(X0-X)PAPB/{P< f'+U)(VAPB/(p' f)+u} It can be shown that only in the case d=3

and dj.=2. i.e. ordinary polymer

After some transformations it takes the more simple form -d c f -p = e fJdu *j 5 (18)

0 {(X0-X)PAPB/{P< f'+U)(VAPB/(p' f)+u} It can be shown that only in the case d=3

and dj.=2. i.e. ordinary polymer

**blends**the dominant part of this integral in the ...### What people are saying - Write a review

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### Contents

Remarks | 2 |

The BaumgartnerMuthukumar Effect in Networks | 11 |

Statistical Mechanics of dDimensional Polymer Networks and Exact | 17 |

Copyright | |

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### Other editions - View all

Molecular Basis of Polymer Networks: Proceedings of the 5th IFF-ILL Workshop ... Artur Baumgärtner,Claude E. Picot No preview available - 2011 |

### Common terms and phrases

42 Molecular Basis anisotropy Basis of Polymer Bastide behaviour blends calculated carrageenan chain segments Chem chemical chemical potential configuration conformation constant constraints corresponding crosslinking curves deformation density dependence deswelling deuterated deviatoric distribution dynamics effect elastic free energy elementary strand elongation entanglements entropy equation equilibrium excluded volume experimental experiments exponent Flory Flory-Huggins Flory-Huggins theory fluctuations fractal dimension free chains free energy Gaussian gelation Gennes helix increases interaction parameter isotropic labelled paths layer length linear Macromolecules macroscopic measurements melt micronetworks modulus molecular weight monomers network chains neutron scattering observed obtained PDMS chains phantom network Phys polybutadiene polyelectrolyte Polymer Networks polymeric fractals polystyrene Proceedings in Physics properties radius of gyration ratio rod network Rouse model rubber elasticity S.F. Edwards sample scaling solution solvent Springer Proceedings star molecules star polymers swelling swollen temperature theory topological uniaxial values vector viscoelastic viscosity volume fraction