Hoffman John D, Lauritzen John I
J Res Natl Bur Stand A Phys Chem. 1961 Jul-Aug;65A(4):297-336. doi: 10.6028/jres.065A.035. Epub 1961 Aug 1.
A systematic study of the problem of spherulitic growth in linear polymers in bulk has been carried out. A calculation of the radial growth of polymer spherulites is given for four models. These concern growth where the surface nuclei that control the rate are (1) bundlelike and coherent, (2) chain folded and coherent, (3) chain folded and noncoherent, and (4) bundlelike and noncoherent. The required modifications of nucleation theory are given. Then the radial growth rate laws are derived for each model, and the type of "spherulite" that would be formed discussed. The model with chain folded and coherent growth nuclei leads to a typical lamellar spherulite. The properties of the individual chain folded lamellae that form the spherulite are predicted, including the change of step height with growth temperature, melting behavior, and the behavior on recrystallization. (Chain folded lamellae may also occur in specimens that are not obviously spherulitic.) Under certain conditions, the noncoherent model with chain folds can lead to a modified lamellar spherulite. None of the bundlelike models will lead to a typical lamellar spherulite, though a spherical microcrystalline object might be formed. It is concluded that lamellar spherulites consist largely of chain folded structures. The factors that could cause chain folded crystals to appear in profusion in bulk polymers are discussed. The case of homogeneous initiation is considered first. Homogeneous initiation of chain folded nuclei in bulk will prevail if the end surface free energy of the bundlelike nucleus exceeds that of the folded. It is shown that the end surface free energy of the bundlelike nucleus, as calculated with a density gradient model, will be larger than had been supposed previously. It is therefore considered to be theoretically possible that the end surface free energy of the bundlelike nucleus may in some cases exceed that of the folded nucleus. Attention is given to the possibility that folded structures appear in large numbers because cumulative strain or large chain ends prevent the growth of bundlelike nuclei to large size, even when the latter type of nucleus is energetically favored when small. Heterogeneous initiation of folded structures is then considered. Other topics mentioned include: (1) Conditions that might lead to nonlamellar or nonspherulitic crystallization in bulk, (2) the origin of the twist that is frequently exhibited by the lamellae in spherulites, (3) the transitions that may sometimes occur in the radial growth rate law, and (4) interlamellar links.
对本体线性聚合物中球晶生长问题进行了系统研究。给出了四种模型下聚合物球晶径向生长的计算。这些模型涉及控制生长速率的表面核为:(1) 束状且连贯;(2) 链折叠且连贯;(3) 链折叠且不连贯;(4) 束状且不连贯。给出了成核理论所需的修正。然后推导了每个模型的径向生长速率定律,并讨论了可能形成的“球晶”类型。具有链折叠且连贯生长核的模型会形成典型的片晶球晶。预测了构成球晶的单个链折叠片晶的性质,包括台阶高度随生长温度的变化、熔化行为以及再结晶行为。(链折叠片晶也可能出现在并非明显呈球晶状的试样中。)在某些条件下,具有链折叠的不连贯模型可导致改性片晶球晶。尽管可能形成球形微晶物体,但束状模型均不会导致典型的片晶球晶。得出结论:片晶球晶主要由链折叠结构组成。讨论了可能导致本体聚合物中大量出现链折叠晶体的因素。首先考虑均相引发情况。如果束状核的端面自由能超过折叠核的端面自由能,则本体中链折叠核的均相引发将占主导。结果表明,用密度梯度模型计算的束状核的端面自由能将比先前设想的更大。因此从理论上认为,在某些情况下束状核的端面自由能可能超过折叠核的端面自由能。关注了折叠结构大量出现的可能性,即累积应变或大的链端阻止束状核生长到较大尺寸,即使在小尺寸时后一种类型的核在能量上更有利。接着考虑折叠结构的非均相引发。提及的其他主题包括:(1) 可能导致本体中出现非片晶或非球晶结晶的条件;(2) 球晶中片晶经常出现的扭曲的起源;(3) 径向生长速率定律有时可能发生的转变;(4) 片晶间连接。