Intrinsic chain stiffness in flexible linear polymers under extreme confinement

Regulation of the gelatin helix-to-coil transition through chain confinements at the polymer-protein interface and protein-protein interface

Gelatin is an essential material widely used in biomedical applications due to its characteristic temperature responsivity-helix-to-coil transition. However, the current helix-to-coil transition is limited by its single-step behavior and the difficulty in designing a specific onset temperature. In this study, we investigated the fundamentals of the helix-to-coil transition with a focus on gelatin chain mobility. We observed distinctive kinetics of the helix-to-coil transition, which is resilient and can actuate in multiple steps or with a controllable onset point. This was achieved by confining the gelatin chain with a hydrophilic polymer or gelatin itself. The confinement approach serves two purposes: first, it prevents excessive mobility of the generated coils, maintaining physical resilience after the helix-to-coil transition; second, the interfacial confinement between the polymer and gelatin, referred to as polymer-protein interface confinement, restricts the helix-to-coil transition, resulting in a multistep transition process. Additionally, strong confinement at the interface between gelatins of different origins, that is protein-protein interface confinement, shifts the onset temperature to a higher point. This fundamental comprehension of helix-to-coil transition could contribute to broadening the biomedical application potential of gelatin materials. STATEMENT OF SIGNIFICANCE: Gelatin is essential in biomedical applications due to its characteristic temperature responsivity-helix-to-coil transition. Herein, we fundamentally investigated the distinctive kinetics of the helix-to-coil transition, which is resilient and can actuate in multiple steps or with a controllable onset point. This was achieved by confining the gelatin chain with a hydrophilic polymer or gelatin itself. The gelatin chain confinement prevents excessive mobility of the generated coils, maintaining physical resilience after the helix-to-coil transition. The interfacial confinement between the polymer and gelatin restricts the helix-to-coil transition, resulting in a multistep transition process. Additionally, strong confinement at the interface between gelatins of different origins shifts the onset temperature to a higher point.

Universal scaling of the osmotic pressure for dense, quasi-two-dimensionally confined polymer melts reveals transitions between fractal dimensions

A scaling law for the osmotic pressure of quasi-two-dimensional polymer melts as a function of concentration is obtained, which shows fractal characteristics. Structural properties such as the chains' contour length and their inner-monomer pair distribution function display fractal scaling properties as well. These predictions are confirmed with mesoscale numerical simulations. The chains are swollen and highly entangled, yet Flory's exponent is always ν = 1/2. The melt can be considered a fluid of "blobs" whose size becomes renormalized in terms of the contour's length while the fractal dimension df increases monotonically between 5/4 and 2, as the monomer concentration is increased. The semidilute scaling of the pressure is recovered when df = 1. Our results agree with recent experiments and with numerical reports on quasi-2d melts. This work provides a new paradigm to study and interpret thermodynamic and structural data in low-dimensional polymer melts, namely as fractal macromolecular objects.

Spatial Organization of Slit-Confined Melts of Ring Polymers with Nonconserved Topology: A Lattice Monte Carlo Study

We present Monte Carlo computer simulations for melts of semiflexible randomly knotted and randomly concatenated ring polymers on the fcc lattice and in slit confinement. Through systematic variation of the slit width at fixed melt density, we explore the influence of confinement on single-chain conformations and interchain interactions. We demonstrate that confinement makes chains globally larger and more elongated while enhancing both contacts and knottedness propensities. As for multichain properties, we show that ring-ring contacts decrease with the confinement, yet neighboring rings overlap more as confinement grows. These aspects are accompanied by a marked decrease in the links formed between pairs of neighboring rings. In connection with the quantitative relation between links and entanglements in polymer melts recently established by us [Ubertini M. A.; Rosa A.Macromolecules2023, 56, 3354-3362], we propose that confinement can be used to set polymer networks that act softer under mechanical stress and suggest a viable experimental setup to validate our results.

Intrinsic structure and dynamics of monolayer ring polymer melts

We present the general structural and dynamical characteristics of flexible ring polymers in narrowly confined two-dimensional (2D) melt systems using atomistic molecular dynamics simulations. The results are further analyzed via direct comparison with the 2D linear analogue as well as the three-dimensional (3D) ring and linear melt systems. It is observed that dimensional restriction in 2D confined systems results in an increase in the intrinsic chain stiffness of the ring polymer. Fundamentally, this arises from an entropic penalty on polymer chains along with a reduction in the available chain configuration states in phase space and spatial choices for individual segmental walks. This feature in combination with the intermolecular interactions between neighboring ring chains leads to an overall extended interpenetrated chain configuration for the 2D ring melt. In contrast to the generally large differences in structural and dynamical properties between ring and linear polymers in 3D melt systems, relatively similar local-to-global chain structures and dynamics are observed for the 2D ring and linear melts. This is attributed to the general structural similarity (i.e., extended double-stranded chain conformations), the less effective role of the chain ends, and the absence of complex topological constraints between chains (i.e., interchain entanglement and mutual ring threading) in the 2D confined systems compared with the corresponding 3D bulk systems.