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Updated: May 22, 2025

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Published on: December 4, 2017
Interface Dynamics of Wet Active Systems
Fernando Caballero1, Ananyo Maitra2,3, Cesare Nardini4,5
1Brandeis University, Department of Physics, Waltham, Massachusetts 02453, USA.
We investigate interface roughening in active suspensions. At large scales, dynamics match the |q|KPZ universality class, even with fluid flow, revealing new insights into active matter systems.
Area of Science:
- Soft Matter Physics
- Active Matter Systems
- Interface Dynamics
Background:
- Phase-separated active suspensions exhibit complex interfacial behavior.
- Understanding interface roughening is crucial for predicting material properties and dynamics.
- Existing models often simplify fluid interactions and substrate effects.
Purpose of the Study:
- To characterize the universality class of interface roughening in active suspensions on substrates.
- To investigate the influence of fluid flow and substrate friction on interfacial dynamics.
- To determine the length scales governing interface randomization.
Main Methods:
- Analysis of interfacial dynamics in phase-separated active suspensions.
- Comparison of experimental or simulation data with theoretical models, specifically the |q|KPZ universality class.
- Examination of early-time dynamics and the impact of system size.
- Investigation of the role of substrate friction and interfacial tension.
Main Results:
- Interfacial dynamics at large length and time scales belong to the |q|KPZ universality class, irrespective of long-ranged fluid flows.
- At early times or in small systems, roughening exponents resemble those in momentum-conserving fluids.
- A de Gennes-Taupin length scale, dependent on interfacial tension, governs interface randomization when substrate friction is negligible.
Conclusions:
- The |q|KPZ universality class accurately describes interface roughening in active suspensions under specific conditions.
- Fluid flow does not alter the large-scale universality class, highlighting robust scaling behavior.
- Substrate friction and interfacial tension play critical roles in determining the randomization length scale of interfaces.
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