We use coarse-grained molecular dynamics simulations to investigate structural organization in melts of brush copolymers as a function of side-chain grafting density, backbone-side-chain miscibility, and backbone rigidity. At low grafting densities, decreasing miscibility drives microphase separation of backbones and side chains and leads to the formation of multi-backbone domains whose morphology evolves from cylindrical aggregates to lamellar structures as the spacer length between grafting points increases. In this regime, the characteristic wavevector q* corresponding to the peak position in the structure factor decreases with increasing the spacer length, reflecting an increase in the domain size. For semiflexible backbones, microphase separation is accompanied by mutual backbone alignment within the multi-backbone domains. Graft copolymers with miscible rigid backbones and flexible side chains can also undergo microphase separation. In this case, the morphological transformations are entropic in origin and are forced by local packing constraints imposed by the flexibility of backbones and side chains and can be viewed as an emergence of local nematic-like ordering of the backbones in a “solvent” of side chains. At high grafting densities, where multiple side chains are attached to each backbone bead, the backbones become effectively screened by the side chains and the melts display smectic-like organization. In this regime, the structure factor develops higher-order peaks at integer multiples of q*. Analysis of orientational correlations of side chain end-to-end vectors confirms that this ordering corresponds to appearance of layers of oriented side chains separating brush backbones. These results establish how graft copolymer architecture, intermolecular interactions, and backbone rigidity govern the transition from microphase-separated comb-like melts to smectic-like ordering in bottlebrush systems.
Introducing charged groups into comb-like copolymers significantly enhances the incompatibility between the main chain and side chains, enabling sub-5 nm microphase separation. In this work, a series of charged comb-like copolymers with imidazolium ionic junctions and mixed alkyl side chains (C18/C8, C20/C12, C22/C12)...
Melt memory in semicrystalline polymers is the remarkable ability of polymer chains to retain structural information from a prior crystalline state after being heated above the melting temperature. This phenomenon can induce extraordinary self-nucleation and strongly influence crystallization kinetics and final materia...
A. de Nicola, A. Müller, Dario Cavallo et al.· Journal of the American Chem...· 0 citations
Melts of semicrystalline homopolymers are classically described as disordered random coils that crystallize into folded-chain lamellar nanocrystals. Here, using ultrahigh-molecular-weight polyethylene (UHMWPE) as a model system, we show that polymerization induces hierarchical ordering that evolves into liquid-crystall...
Aizezi Maimaitiming, Kun Cui, Feng Tian et al.· Materials Horizons· 0 citations
Atomistic nonequilibrium molecular dynamics simulations of entangled polydisperse polyethylene melts possessing a realistic log-normal molecular-weight distribution under planar elongational flow demonstrate that polydispersity fundamentally modifies the coil–stretch transition (CST). In contrast to the sharp, bi-direc...
Elyar Tourani, M. N. Sefiddashti, Brian J. Edwards et al.· Journal of rheology· 0 citations
Semicrystalline polymers are often idealized as forming lamellar stacks with an average long period (d-spacing) varying little throughout the specimen. In this work, two distinct types of lamellar stack, each with a different d-spacing and melting temperature, were observed in hydrogenated poly(norbornene-r-hexylnorb...
Katherine M. Gunter, Gracyn M. Reynolds, R. Register· Macromolecules· 0 citations