Molecular understanding for large deformations of soft bottlebrush polymer networks

Abstract

Networks formed by crosslinking bottlebrush polymers are a class of soft materials with stiffnesses matching that of ‘watery’ hydrogels and biological tissues but contain no solvents. Because of their extreme softness, bottlebrush polymer networks are often subject to large deformations. However, it is poorly understood how molecular architecture determines the extensibility of the networks. Using a combination of experimental and theoretical approaches, we discover that the yield strain γ_y of the network equals the ratio of the contour length L_max to the end-to-end distance R of the bottlebrush between two neighboring crosslinks: γ_y = L_max/R − 1. This relation suggests two regimes: (1) for stiff bottlebrush polymers, γ_y is inversely proportional to the network shear modulus G, γ_y ∼ G⁻¹, which represents a previously unrecognized regime; (2) for flexible bottlebrush polymers, γ_y ∼ G^−1/2, which recovers the behavior of conventional polymer networks. Our findings provide a new molecular understanding of the nonlinear mechanics for soft bottlebrush polymer networks.