Polymorphism of stable collagen fibrils

TL;DR

This study models collagen fibril configurations using a liquid crystal approach, revealing how elastic and surface tension parameters determine fibril radius and surface twist, explaining variations in biological tissues.

Contribution

It introduces a thermodynamic model that predicts stable collagen fibril structures based on elastic constants and surface tension ratios, linking physical parameters to biological fibril diversity.

Findings

Stable fibril configurations depend on elastic and surface tension ratios.

Large surface twist explains narrow corneal fibril radius distribution.

Small surface twist stabilizes tendon fibrils despite radius polydispersity.

Abstract

Collagen fibrils are versatile self-assembled structures that provide mechanical integrity within mammalian tissues. The radius of collagen fibrils vary widely depending on experimental conditions \textit{in vitro} or anatomical location \textit{in vivo}. Here we explore the variety of thermodynamically stable fibril configurations that are available. We use a liquid crystal model of radial collagen fibril structure with a double-twist director field. Using a numerical relaxation method we show that two dimensionless parameters, the ratio of saddle-splay to twist elastic constants $ k_{24}/K_{22}$ and the ratio of surface tension to chiral strength $\hat{\gamma} \equiv \gamma/(K_{22}q)$, largely specify both the scaled fibril radius and the associated surface twist of equilibrium fibrils. We find that collagen fibrils are the stable phase with respect to the cholesteric phase only when the reduced surface tension is small, $\hat{\gamma} \lesssim 0.2$. Within this stable regime, collagen fibrils can access a wide range of radii and associated surface twists. Remarkably, we find a maximal equilibrium surface twist of $0.33$ rad ($19^{\text{o}}$). Our results are compatible with corneal collagen fibrils, and we show how the large surface twist is needed to explain the narrow distribution of corneal fibril radii. Conversely, we show how small surface twist is required for the thermodynamic stability of tendon fibrils in the face of considerable polydispersity of radius.