Schnell B, Meyer H, Fond C, Wittmer J P, Baschnagel J
Institut Charles Sadron, Université de Strasbourg, CNRS UPR 22, 23 rue du Loess-BP 84047, 67034 Strasbourg Cedex 2, France.
Eur Phys J E Soft Matter. 2011 Sep;34(9):97. doi: 10.1140/epje/i2011-11097-4. Epub 2011 Sep 23.
By means of molecular-dynamics simulation we study a flexible and a semiflexible bead-spring model for a polymer melt on cooling through the glass transition. Results for the glass transition temperature T(g) and for the elastic properties of the glassy state are presented. We find that T(g) increases with chain length N and is for all N larger for the semiflexible model. The N dependence of T(g) is compared to experimental results from the literature. Furthermore, we characterize the polymer glass below T(g) via its elastic properties, i.e., via the Lamé coefficients λ and μ. The Lamé coefficients are determined from the fluctuation formalism which allows to split λ and μ into affine (Born term) and nonaffine (fluctuation term) contributions. We find that the fluctuation term represents a substantial correction to the Born term. Since the Born terms for λ and μ are identical, the fluctuation terms are responsible for the different temperature dependence of the Lamé coefficients. While λ decreases linearly on approaching T(g) from below, the shear modulus μ displays a much stronger decrease near T(g). From the present simulation data it is not possible to decide whether μ takes a finite value at T(g), as would be expected from mode-coupling theory, or vanishes continuously, as suggested by recent work from replica theory.
通过分子动力学模拟,我们研究了聚合物熔体在冷却通过玻璃化转变时的柔性和半柔性珠簧模型。给出了玻璃化转变温度(T(g))以及玻璃态弹性性质的结果。我们发现(T(g))随链长(N)增加,并且对于所有(N),半柔性模型的(T(g))都更大。将(T(g))对(N)的依赖性与文献中的实验结果进行了比较。此外,我们通过聚合物玻璃低于(T(g))时的弹性性质,即通过拉梅系数(\lambda)和(\mu)来表征它。拉梅系数由涨落形式理论确定,该理论允许将(\lambda)和(\mu)分为仿射(玻恩项)和非仿射(涨落项)贡献。我们发现涨落项对玻恩项是一个实质性的修正。由于(\lambda)和(\mu)的玻恩项相同,涨落项导致了拉梅系数不同的温度依赖性。当从下方接近(T(g))时,(\lambda)线性下降,而剪切模量(\mu)在(T(g))附近下降得更强。从目前的模拟数据无法确定(\mu)在(T(g))时是否取有限值,这是模式耦合理论所预期的,还是如副本理论最近的工作所暗示的那样连续消失。