Uncovering the Microscopic Origin of Fluidization

Figure 1: The formation of stress granules in human cells upon the addition of Sodium Arsenite. Green regions show the location of G3BP, a protein which is known to localise in stress granules. Scale bar: 20 μm. Copyright: Published in Law J. O. et. al., Sci. Adv., 9, eadg0432 (2023) under a Creative Commons Attribution 4.0 International License.
Unlocking Cell Secrets with Flicker Spectroscopy
27th January 2025

The SoftComp partner CNRS Montpellier, France (Laboratory Charles Coulomb Laboratory, CNRS and University of Montpellier) and the Center for Soft Matter Research at New York University have shed light on the microscopic origin of fluidization, a phenomenon where complex fluids transition from a solid-like state to a flowing state when subjected to external forces.

To achieve this, the team studied concentrated colloidal suspensions and emulsions, soft and amorphous solids made up of micron-sized particles or droplets, highly compressed and dispersed in a solvent. They employed a novel approach, illuminating the samples with a laser while applying cyclic shear deformation. By analysing the temporal fluctuations of the light scattered by the samples, the researchers established a link between the sample’s macroscopic mechanical deformation and a transition between two distinct microscopic dynamic states of matter, characteristic of solid and fluid behaviours.

The modelling of the experimental results was inspired by the work of Dutch physicist J.D. van der Waals, who over a century ago explained the transition between equilibrium states from liquid to gas phase. By adapting van der Waals’ concepts to their systems, the scientists proposed a model in which the dynamics of adjacent regions of a soft solid subjected to shear are coupled, in the same way van der Waals molecules interact with each other, while the amplitude of the imposed deformation plays the same role as depressurization in simple liquids.

 
Figure: Unified state diagram for the fluidization transition. For small deformation amplitudes, soft systems exhibit solid-like dynamics (blue points) with low fluidity, namely very large spontaneous relaxation times. As the deformation amplitude increases, soft systems undergo the fluidization transition (gray points), characterized by the coexistence of two types of dynamics (solid and fluid). They are eventually fluidized at very large deformations, where the microscopic dynamics resemble those of a liquid. (Copyright © 2023: the authors)
Figure: Unified state diagram for the fluidization transition. For small deformation amplitudes, soft systems exhibit solid-like dynamics (blue points) with low fluidity, namely very large spontaneous relaxation times. As the deformation amplitude increases, soft systems undergo the fluidization transition (gray points), characterized by the coexistence of two types of dynamics (solid and fluid). They are eventually fluidized at very large deformations, where the microscopic dynamics resemble those of a liquid. (Copyright © 2023: the authors)

This led to an equation that is formally identical to van der Waals’ famous equation of state for real gases, opening the way for a unified phase diagram for the fluidization transition. The  results of this study provide new insights into the microscopic origin of fluidization, reconciling previously contrasting observations and paving the way for further research and innovations in fields such as materials science, engineering, and biotechnology.

Read more:
Aime S. et al., Nat. Phys. 19, 1673 (2023)

SoftComp partner:
CNRS Montpellier (Laboratory Charles Coulomb Laboratory in France, CNRS and University of Montpellier) 

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