Titlebook: Ordering in Macromolecular Systems; Proceedings of the O Akio Teramoto,Masamichi Kobayashi,Takashi Norisuye Conference proceedings 1994 Spr

艦旗

Supramolecular Assemblies of Cyclodextrins with Polymers and Preparation of Polyrotaxanes,talline states. α-CD formed complexes with poly(ethylene glycol)(PEG) of molecular weight higher than 300, although β-CD did not form complexes with PEG of any molecular weight. However, β-CD formed complexes with poly(propylene glycol)(PPG), although α-CD did not form complexes with PPG of any mole

整潔

Case II Diffusion in Polystyrene Fiber: , Measurement of a Moving Sharp Front,ng technique. The diffusion of acetone vapor with the relative vapor pressure of 0.92 into the physically aged polystyrene fiber of 25 .m diameter was measured at 25°C. The system showed following characteristics; (1) an induction time, (2) formation of a sharp front after the induction time, (3) ne

Factorable

,“Liquid Crystallization” Mechanism of Liquid Crystalline Polymers, their formation mechanism was studied. Materials used were a copolyether based on 1,2-Bis (4-hydroxy phenyl) ethane (BPE-8/12) and poly [bis (trifluoro ethoxy) phosphazenel, (PBFP). Morphology of liquid crystals observed by polarizing microscopy and that of the quenched liquid crystals into crystal

迫擊炮

cacophony

Limited

疼死我了

antiquated

Default

,Light Scattering Studies of a Nematic to Smectic — A Phase Transition in Rigid Rod Polymer Solutionard repulsion, rather than the complicated interparticle potentials found in most liquid crystals. Computer simulations have shown [1] that a nematic to smectic A phase transition may exist in a system as simple as monodisperse hard rods. Experimentally, Xin Wen, Robert Meyer and Donald Caspar [2] h

事情

Collective and Molecular Dynamics in Ferroelectric Liquid Crystals: From Low Molar to Polymeric andelectric liquid crystals (FLC). Below 10.Hz two collective dielectric relaxation processes are observed having the character of a soft — mode and that of a Goldstone — mode. The soft — mode is assigned to fluctuations of the amplitude of the helical superstructure, while the Goldstone — mode corresp