Shape variation of linear polymers upon phase separation in a ternary solution
Shape variation of linear polymers upon phase separation in a ternary solution
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DOI:
10.1021/ma034506o
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发表时间:
2003-10-21
期刊:
影响因子:
5.5
通讯作者:
Luijten, E
中科院分区:
文献类型:
--
作者:
Guo, L;Luijten, E
It was recognized by Kuhn 70 years ago that the typical shape of a flexible polymer chain is ellipsoidal rather than spherical. 1 This shape anisotropy, besides being a fundamental property, is of considerable scientific and technological importance, affecting a variety of polymer properties. For example, it has been proposed that it influences the flow properties of polymeric fluids, 2 and recently it was demonstrated3 that the polymer asphericity can account for the polymer-induced depletion potential observed in colloid-polymer mixtures. 4 Accordingly, the shape of random-walk (RW) and selfavoiding-walk (SAW) polymers has been studied extensively both analytically and by simulations. 5-9 Very recently, the asymmetric shape has actually been observed in experiments. 10, 11 However, it should be noted that the experiments, as well as the vast majority of the theoretical work, focus on the shape of a single coil in a highly dilute solution. Studies of the role of concentration are rare and have essentially shown that, for a homogeneous solution of athermal chains, the asphericity diminishes only very slowly upon increasing concentration. 12, 13 In a poor solvent, the reverse effect was observed, 14 which is essentially due to the coil-globule transition taking place in the polymer-lean phase. Clearly, structural and thermodynamic properties are intimately connected, which has motivated us to investigate shape variations within a more complicated phase diagram. In this Note, we discuss the coil shapes of polymers in a ternary solution, consisting of two polymer species (denoted by A and B) and a solvent (S). In particular, we focus on the effect of polymer-polymer separation in this system, which we have investigated by means of Monte Carlo simulations. It is found that this phase transition indeed has a dramatic effect on the polymer shape, which is characterized by the eigenvalues λ1 e λ2 e λ3 of the radius-of-gyration tensor Q, defined as5, 15 where ri represents the position of the ith monomer along the chain, R,) 1, 2, 3 denote Cartesian components, and N is the degree of polymerization of the polymer. The sum of the three eigenvalues equals the squared radius of gyration Rg 2. An important measure is the asphericity A6, 9, 16, 17 where the brackets indicate the ensemble average. 18 A takes values between 0 (sphere) and 1 (rod). In the dilute limit it approaches a universal value for N f∞, estimated as 0.415 from first-order ϵ expansions and as 0.431 from simulations. 9, 19, 20 In the melt limit, where the chains behave ideally, this value is anticipated to decrease to the (exactly known) RW value 0.39427.... 17