Monte Carlo simulation of polymer welding

被引:19
作者
Haire, KR [1 ]
Windle, AH [1 ]
机构
[1] Univ Cambridge, Dept Mat Sci & Met, Cambridge CB2 3QZ, England
来源
COMPUTATIONAL AND THEORETICAL POLYMER SCIENCE | 2001年 / 11卷 / 03期
关键词
Monte Carlo modelling; polymer welding; reptation theory;
D O I
10.1016/S1089-3156(00)00011-8
中图分类号
O63 [高分子化学(高聚物)];
学科分类号
070305 ; 080501 ; 081704 ;
摘要
Monte Carlo Modelling of random polymer chains, course grained onto a cubic F lattice, provides the ability to monitor the long range relaxation processes and the dynamic parameters of chains up to 400 units long. The model, described and verified by Haire et al. (Haire KR, Carver TJ, Windle AK. A Monte Carlo model for dense polymer systems and its interlocking with molecular dynamics simulation. Computational and Theoretical Polymer Science 2000; in press), is here applied to the study of molecular parameters in the vicinity of different types of surface and also to the process of polymer welding, whereby adhesion between two adjacent surfaces is achieved by the interpenetration of chains which are across the surface. The model demonstrates that a surface distorts the conformation of chains adjacent to it to give an oblate molecular envelope, that the concentration of vacant sites and chain ends increases near to the surface and that the density of points representing the centres of mass of the chains increases in the sub-surface regions. These results confirm earlier predictions and provide additional confidence in the model. Modelling of the welding process leads to the parameter intrinsic weld time, t(w), which is the time from initial perfect contact of the surfaces to the achievement of a weld within which the chain conformation is indistinguishable from the bulk. After the initial period in which the mating surfaces roughen, the welding proceeds according to the t(1/4) law predicted by reptation theory. The time to a given level of interdiffusion across the boundary is proportional to the chain length I, a comparatively weak dependence, while t(w) is proportional to l(3), a strong dependence. This is the same dependence on length as for the relaxation time of the chain end-to-end vectors. In fact, the agreement between the relaxation time, measured on the model of the bulk, and t(w) is surprisingly close, at least for the monodisperse polymers investigated here. (C) 2000 Elsevier Science Ltd. All rights reserved.
引用
收藏
页码:227 / 240
页数:14
相关论文
共 14 条
[1]   Interfacial properties of glassy polymer melts: A Monte Carlo study [J].
Baschnagel, J ;
Binder, K .
MACROMOLECULAR SYMPOSIA, 1996, 106 :41-54
[2]  
HAIRE KR, 2000, IN PRESS COMPUTATION
[3]   MONTE-CARLO SIMULATIONS OF THE FREE-SURFACE OF POLYMER MELTS [J].
KUMAR, SK ;
RUSSELL, TP ;
HARIHARAN, A .
CHEMICAL ENGINEERING SCIENCE, 1994, 49 (17) :2899-2906
[4]   STRUCTURAL AND THERMODYNAMIC PROPERTIES OF INTERFACES BETWEEN COEXISTING PHASES IN POLYMER BLENDS - A MONTE-CARLO SIMULATION [J].
MULLER, M ;
BINDER, K ;
OED, W .
JOURNAL OF THE CHEMICAL SOCIETY-FARADAY TRANSACTIONS, 1995, 91 (16) :2369-2379
[5]   COMPUTER-SIMULATION OF POLYMERS IN THIN-LAYERS .1. POLYMER MELT BETWEEN NEUTRAL WALLS-STATIC PROPERTIES [J].
PAKULA, T .
JOURNAL OF CHEMICAL PHYSICS, 1991, 95 (06) :4685-4690
[6]   MONTE-CARLO SIMULATION OF LATTICE MODELS FOR MACROMOLECULES AT HIGH-DENSITIES [J].
REITER, J ;
EDLING, T ;
PAKULA, T .
JOURNAL OF CHEMICAL PHYSICS, 1990, 93 (01) :837-844
[7]   Direct correlation between interfacial width and adhesion in glassy polymers [J].
Schnell, R ;
Stamm, M ;
Creton, C .
MACROMOLECULES, 1998, 31 (07) :2284-2292
[8]   Interdiffusion of deuterated and protonated poly(methyl methacrylate) [J].
Shearmur, TE ;
Clough, AS ;
Drew, DW ;
van der Grinten, MGD ;
Jones, RAL .
POLYMER, 1998, 39 (11) :2155-2159
[9]   Dynamics of polymer interdiffusion: The ripple experiment [J].
Welp, KA ;
Wool, RP ;
Satija, SK ;
Pispas, S ;
Mays, J .
MACROMOLECULES, 1998, 31 (15) :4915-4925
[10]   A THEORY OF CRACK HEALING IN POLYMERS [J].
WOOL, RP ;
OCONNOR, KM .
JOURNAL OF APPLIED PHYSICS, 1981, 52 (10) :5953-5963