DYNAMIC VISCOELASTICITY OF END-LINKING ALPHA,OMEGA-DIMETHYL SILYL POLY(PROPYLENE OXIDE) SOLUTIONS NEAR THE GEL POINT

被引:55
作者
KOIKE, A
NEMOTO, N
TAKAHASHI, M
OSAKI, K
机构
[1] KYOTO UNIV, INST CHEM RES, UJI, KYOTO 611, JAPAN
[2] KYOTO UNIV, DIV MAT CHEM, KYOTO 606, JAPAN
[3] KYUSHU UNIV, DEPT APPL SCI, FUKUOKA 812, JAPAN
关键词
DYNAMIC VISCOELASTICITY; END-LINKING POLYMER; GELATION;
D O I
10.1016/0032-3861(94)90413-8
中图分类号
O63 [高分子化学(高聚物)];
学科分类号
070305 ; 080501 ; 081704 ;
摘要
Dynamic viscoelasticity of alpha,omega-dimethyl silyl poly(propylene oxide) solutions was studied through the gelation process with end-linking. The gel point was determined as the reaction time, t=t(c), at which the storage and the loss shear moduli, G'(omega) and G'(omega)), respectively, both became proportional to omega(n) over the whole omega range measured, where omega is the angular frequency and n is a constant. Effects of polymer molecular weight M and concentration c on the steady-state viscosity eta before the gel point and the equilibrium modulus G(eq) after the gel point were examined in terms of critical exponents, k and z, defined by power laws, eta approximately (\t - t(c)\/t(c))-k is similar to epsilon(-k) and G(eq) is similar to epsilon(z), respectively (s being the relative distance from the gel point). The three exponents n, k and z were found to take universal values of n = 0.66 +/- 0.02, k = 1.0 +/- 0.1 and z = 2.0 +/- 0.1 irrespective of M and c for unentangled systems. In these systems, the reduced plot of G(eq)(epsilon)/G(infinity) versus epsilon gave a single composite curve in the range of 0.1 < epsilon < 0.7, where G(infinity) was the modulus for the ideal network in which all functional groups reacted. The presence of entanglement coupling in the prepolymer solutions made the critical behaviour of eta and G(eq) obscure and affected the exponent values. The results were briefly compared with theoretical predictions.
引用
收藏
页码:3005 / 3010
页数:6
相关论文
共 41 条
[1]   MECHANICAL MEASUREMENTS IN THE REACTION BATH DURING THE POLYCONDENSATION REACTION, NEAR THE GELATION THRESHOLD [J].
ADAM, M ;
DELSANTI, M ;
DURAND, D .
MACROMOLECULES, 1985, 18 (11) :2285-2290
[2]   DYNAMICAL STUDIES OF POLYMERIC CLUSTER SOLUTIONS OBTAINED NEAR THE GELATION THRESHOLD - GLASSLIKE BEHAVIOR [J].
ADAM, M ;
DELSANTI, M ;
MUNCH, JP ;
DURAND, D .
PHYSICAL REVIEW LETTERS, 1988, 61 (06) :706-709
[3]   EVOLUTION OF STRUCTURE AND VISCOELASTICITY IN AN EPOXY NEAR THE SOL-GEL TRANSITION [J].
ADOLF, D ;
MARTIN, JE ;
WILCOXON, JP .
MACROMOLECULES, 1990, 23 (02) :527-531
[4]   MICRONETWORKS BY END-LINKING OF POLYSTYRENE .2. DYNAMIC MECHANICAL-BEHAVIOR AND DIFFUSION EXPERIMENTS IN THE BULK [J].
ANTONIETTI, M ;
FOLSCH, KJ ;
SILLESCU, H ;
PAKULA, T .
MACROMOLECULES, 1989, 22 (06) :2812-2817
[5]   LINEAR VISCOELASTICITY AT THE GEL POINT OF A CROSS-LINKING PDMS WITH IMBALANCED STOICHIOMETRY [J].
CHAMBON, F ;
WINTER, HH .
JOURNAL OF RHEOLOGY, 1987, 31 (08) :683-697
[6]  
CHAMBON F, 1985, POLYM BULL, V13, P499
[7]   RHEOLOGY OF MODEL POLYURETHANES AT THE GEL POINT [J].
CHAMBON, F ;
PETROVIC, ZS ;
MACKNIGHT, WJ ;
WINTER, HH .
MACROMOLECULES, 1986, 19 (08) :2146-2149
[8]  
de Gennes P.-G, 1979, SCALING CONCEPTS POL
[9]   GELATION OF COLLOIDAL SILICA [J].
DIETLER, G ;
AUBERT, C ;
CANNELL, DS ;
WILTZIUS, P .
PHYSICAL REVIEW LETTERS, 1986, 57 (24) :3117-3120
[10]   FREQUENCY-DEPENDENCE OF VISCOELASTIC PROPERTIES OF BRANCHED POLYMERS NEAR GELATION THRESHOLD [J].
DURAND, D ;
DELSANTI, M ;
ADAM, M ;
LUCK, JM .
EUROPHYSICS LETTERS, 1987, 3 (03) :297-301