Marencic Andrew P, Adamson Douglas H, Chaikin Paul M, Register Richard A
Department of Chemical Engineering, Princeton University, Princeton, New Jersey 08544, USA.
Phys Rev E Stat Nonlin Soft Matter Phys. 2010 Jan;81(1 Pt 1):011503. doi: 10.1103/PhysRevE.81.011503. Epub 2010 Jan 21.
In common with many other structured fluids, block copolymers can be effectively oriented by shear. This susceptibility to shear alignment has previously been shown to hold even in thin films, containing as few as two layers of spherical microdomains, or even a single layer of cylindrical microdomains. A phenomenological model has been proposed [M. W. Wu, R. A. Register, and P. M. Chaikin, Phys. Rev. E 74, 040801(R) (2006)] to describe the alignment of such block-copolymer films, yielding the microdomain lattice order parameter as a function of shearing temperature, stress, and time. Here we directly test the central idea of that model, that the grains which are most misaligned with the shear direction are selectively destroyed, to reform in a direction more closely aligned with the shear. Films are first shear aligned from a polygrain state into a monodomain orientation and are then subjected to a second shear, at a variable stress (sigma) and misorientation angle (deltatheta) relative to the monodomain director, allowing the effects of sigma and deltatheta to be independently and systematically probed. For both cylinder-forming and sphere-forming block copolymers, these experiments confirm the basic premise of the model, as the stress required for realignment increases monotonically as deltatheta becomes smaller. For a cylinder-forming block copolymer, we find that the characteristic stress sigma(c) required to realign cylinders from one monodomain orientation to another is indistinguishable from that required to generate a monodomain orientation from the polygrain state. By contrast, the hexagonal lattice of spheres requires a value of sigma(c) more than 3 times as high for reorientation than for generation of the initial monodomain orientation.
与许多其他结构化流体一样,嵌段共聚物可以通过剪切有效地取向。先前已表明,即使在薄膜中,这种对剪切取向的敏感性依然存在,这些薄膜中包含少至两层的球形微区,甚至单层的圆柱形微区。已经提出了一个唯象模型[M. W. 吴、R. A. 雷吉斯特和P. M. 柴金,《物理评论E》74, 040801(R) (2006)]来描述这种嵌段共聚物薄膜的取向,得出微区晶格序参量作为剪切温度、应力和时间的函数。在此,我们直接测试该模型的核心观点,即与剪切方向最不一致的晶粒会被选择性破坏,从而在更接近与剪切方向一致的方向上重新形成。首先将薄膜从多晶态剪切取向为单畴取向,然后相对于单畴指向矢在可变应力(σ)和取向差角(Δθ)下进行第二次剪切,从而能够独立且系统地探究σ和Δθ的影响。对于形成圆柱状和球状的嵌段共聚物,这些实验都证实了该模型的基本前提,因为随着Δθ变小,重新取向所需的应力单调增加。对于一种形成圆柱状的嵌段共聚物,我们发现将圆柱从一个单畴取向重新取向到另一个单畴取向所需的特征应力σ(c)与从多晶态生成单畴取向所需的应力并无区别。相比之下,球状的六角晶格重新取向所需的σ(c)值比生成初始单畴取向所需的值高出3倍以上。