Concentration Dependence of Elastic and Viscoelastic Properties of Aqueous Solutions of Ficoll and Bovine Serum Albumin by Brillouin Light Scattering Spectroscopy

TL;DR

This study investigates how the elastic and viscoelastic properties of Ficoll and BSA aqueous solutions change with concentration using Brillouin light scattering, revealing interactions and bound water effects.

Contribution

It provides new insights into concentration-dependent elastic and viscoelastic properties of Ficoll and BSA solutions, highlighting intermolecular interactions and bound water effects.

Findings

Linear spectral shifts at low concentrations

Quadratic dependence indicating intermolecular interactions

Evidence of bound water exchange in Ficoll solutions

Abstract

The cellular environment is crowded with macromolecules of different shapes and sizes. The effect of this macromolecular crowding has been studied in a variety of synthetic crowding environments: two popular examples are the compact colloid-like Ficoll macromolecule, and the globular protein bovine serum albumin (BSA). Recent studies have indicated a significant component of bound or surface-associated water in these crowders reduces the available free volume. In this work, Brillouin light scattering experiments were performed on aqueous solutions of Ficoll 70 and Ficoll 400 with concentrations ranging from 1 wt% to 35 wt% and BSA with concentrations of 1 wt% to 27 wt%. From the dependence of spectral peak parameters on polymer concentration, we determined fundamental solution properties: hypersound velocity, adiabatic bulk modulus and compressibility, apparent viscosity, and hypersound attenuation. Existing theory that ignores intermolecular interactions can only capture the observed linear trends in the frequency shift up to a threshold concentration, beyond which a quadratic term accounting for intermolecular interactions is necessary. This likely indicates a transition from the dilute to semi-dilute regime. In the Ficoll solutions (but not BSA) we see evidence for a central mode, with a characteristic relaxation time of 20 ps, that we attribute to exchange of the bound water.