OSMOTIC-PRESSURE, ATOMIC PRESSURE AND THE VIRIAL EQUATION OF STATE OF POLYMER-SOLUTIONS - MONTE-CARLO SIMULATIONS OF A BEAD-SPRING MODEL

被引:51
作者
MILCHEV, A
BINDER, K
机构
[1] UNIV MAINZ,INST PHYS,D-55099 MAINZ,GERMANY
[2] BULGARIAN ACAD SCI,INST PHYS CHEM,BU-1040 SOFIA,BULGARIA
关键词
D O I
10.1002/mats.1994.040030601
中图分类号
O63 [高分子化学(高聚物)];
学科分类号
070305 ; 080501 ; 081704 ;
摘要
A recently introduced coarse-grained model of polymer chains is studied analyzing various contributions to the pressure as obtained from the virial theorem as a function of chain length N, temperature T and density phi. The off-lattice model of the polymer chains has anharmonic springs between the beads, bur of finite extensibility, and the Morse-type interaction between beads is repulsive at very short distances and attractive at intermediate distances. Solvent molecules are not explicitly included. It is found that the covalent forces along the chain (modelled by the spring potentials) contribute a negative term to the pressure, irrespective of temperature, which vanishes linearly in phi as phi --> 0. In contrast, both contributions to the pressure due to intrachain nonbonded forces and due to forces between different chains change sign Born high temperatures (T >> theta, theta the theta-temperature) where they are positive, to low temperature where both parts of the pressure become negative. It is shown that the total pressure has the expected behavior with temperature near the theta-temperature, i.e., Delta p = p(tot) - k(B).T rho similar to (T - theta). We study also the concentration and chainlength dependence of the various contributions to the pressure in the good solvent regime and interpret them with scaling predictions.
引用
收藏
页码:915 / 929
页数:15
相关论文
共 84 条
[21]   LAGRANGIAN THEORY OF POLYMER-SOLUTIONS AT INTERMEDIATE CONCENTRATIONS [J].
DESCLOIZEAUX, J .
JOURNAL DE PHYSIQUE, 1975, 36 (04) :281-291
[22]   INTERDIFFUSION AND SELF-DIFFUSION IN POLYMER MIXTURES - A MONTE-CARLO STUDY [J].
DEUTSCH, HP ;
BINDER, K .
JOURNAL OF CHEMICAL PHYSICS, 1991, 94 (03) :2294-2304
[23]   EQUATION OF STATE FOR ATHERMAL LATTICE CHAINS IN A 3D FLUCTUATING BOND MODEL [J].
DEUTSCH, HP ;
DICKMAN, R .
JOURNAL OF CHEMICAL PHYSICS, 1990, 93 (12) :8983-8990
[24]   EQUATION OF STATE OF 2-DIMENSIONAL LATTICE CHAINS AT THE THETA POINT [J].
DICKMAN, R .
JOURNAL OF CHEMICAL PHYSICS, 1992, 96 (02) :1516-1522
[25]   EQUATION OF STATE FOR CHAIN MOLECULES - CONTINUOUS-SPACE ANALOG OF FLORY THEORY [J].
DICKMAN, R ;
HALL, CK .
JOURNAL OF CHEMICAL PHYSICS, 1986, 85 (07) :4108-4115
[27]   HIGH-DENSITY MONTE-CARLO SIMULATIONS OF CHAIN MOLECULES - BULK EQUATION OF STATE AND DENSITY PROFILE NEAR WALLS [J].
DICKMAN, R ;
HALL, CK .
JOURNAL OF CHEMICAL PHYSICS, 1988, 89 (05) :3168-3174
[28]   NEW SIMULATION METHOD FOR THE EQUATION OF STATE OF LATTICE CHAINS [J].
DICKMAN, R .
JOURNAL OF CHEMICAL PHYSICS, 1987, 87 (04) :2246-2248
[29]   ROLE OF MOLECULAR-STRUCTURE ON THE THERMODYNAMIC PROPERTIES OF MELTS, BLENDS, AND CONCENTRATED POLYMER-SOLUTIONS - COMPARISON OF MONTE-CARLO SIMULATIONS WITH THE CLUSTER THEORY FOR THE LATTICE MODEL [J].
DUDOWICZ, J ;
FREED, KF ;
MADDEN, WG .
MACROMOLECULES, 1990, 23 (22) :4803-4819
[30]  
Flory P. J., 1953, PRINCIPLES POLYM CHE