Search arXivSearch

arXiv · 2412.00972

Aggregation of hydrophobic-amphiphilic block copolymers

Abstract

We analyze the aggregation of locally amphiphilic copolymers with blocky architecture and uniformly distributed amphiphilic moieties in terms of a mean-field theory. Locally amphiphilic structure is characteristic of many thermoresponsive polymers, both linear and grafted, which endows them with local surface activity. Self-assembly of such copolymers exhibits a rich diversity of morphologies, which are analyzed in the present work in the limit of high surface activity of amphiphilic dimers with solvophilic/polar pendants. Depending on the composition and architecture of the copolymer and sizes and interaction parameters of the solvophilic/polar pendants, we build morphological diagrams of copolymer solutions. Copolymers with small volume pendants form precipitates or large aggregates with internal voids containing these pendants. For moderate volume pendants, a lamellar structure (or large vesicles) is observed at smaller fractions of amphiphilic monomer units in the chain and micelles are formed at larger fractions of these units. The sizes and shapes of micelles depend on the monomer distribution along the chain, and the blocky architecture favors the existence of single spherical micelles or spherical particles that constitute compound micelles. For sufficiently large polar pendants, copolymers of both types mainly form granular branched compound micelles. The distance at which adjacent hydrophobic and polar groups are located in a chain determines the size of domains and particles formed by locally amphiphilic blocks or chains. Our predictions explain the existence of dense multicore complex micelles consisting of beads of several tens of nanometers size and other structures such as disc-shaped micelles.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

S. A. Pavlenko, E. N. Govorun. 2024-12-28. Aggregation of hydrophobic-amphiphilic block copolymers. https://arxiv.org/abs/2412.00972

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Deformation and organization of droplet-encapsulated soft beads

Many biological, culinary, and engineering processes lead to the co-encapsulation of several soft particles within a liquid interface. In these situations the particles are bound together by the capillary forces that deform them and influence their biological or rheological properties. Here, we introduce an experimental approach to encapsulate a controlled number of soft beads within aqueous droplets in oil. These droplet-encapsulated gels are manipulated in a deformable microfluidic device to merge them and modify the liquid fraction. In the dry limit the contact surface between the hydrogels is found to be determined by the elastocapillary number $E_c$, with the contact radius following a $E_c^{1/3}$ dependence, indicating that the deformation increases for soft or small particles. When multiple beads are co-encapsulated within a single droplet they can be arranged into linear or three-dimensional aggregates that remain at a local energy minimum.

cond-mat.soft

Flexoelectricity-driven softening of bend elasticity leads to spontaneous chiral symmetry breaking in a polar fluid

The origin of the recently observed spontaneous chiral symmetry breaking in polar fluids composed of achiral molecules is an unsolved problem, raising fundamental questions about how heliconical structures emerge in such systems. Here, we investigate the pretransitional fluctuations leading to the formation of the spontaneously chiral twist-bend ferroelectric nematic phase using dielectric spectroscopy, light scattering, and small-angle X-ray scattering. We observe simultaneous softening of the bend elastic constant and the emergence of a collective dielectric mode on approaching the transition. By developing a theoretical model, we show that these phenomena are signatures of a flexoelectricity-driven transition arising from the coupling between electric polarization and bend deformation.

cond-mat.soft

Taylor dispersion in a soft tube

Diffusion of a solute along a tube is enhanced by hydrodynamic flow, a phenomenon known as Taylor dispersion. In microfluidic applications, the compliance of the tube boundaries modifies the hydrodynamic flow and thus solutal transport. Here, we develop the theory of solutal dispersion in a soft, axisymmetric tube where the tube walls respond to the hydrodynamic pressure through a Winkler response. By deriving the modified macro-transport equation for the solutal concentration dynamics based on multiple-time-scale analysis, we explore the influence of softness on solutal transport for steady and pulsatile configurations. Our main finding is that softness enhances the effective advection velocity and dispersion coefficient, which might have practical implication in biology and microfluidic technology.

cond-mat.soft