Related Experiment Video
Updated: Oct 20, 2025

06:37
Analyzing Melts and Fluids from Ab Initio Molecular Dynamics Simulations with the UMD Package
Published on: September 17, 2021
4.7K
Thermally activated flow in models of amorphous solids
Marko Popović1, Tom W J de Geus1, Wencheng Ji1
1Institute of Physics, École Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland.
Physical Review. E
|September 16, 2021
Summary
Amorphous solids exhibit thermally activated flow below a critical stress. This study presents a general scaling law describing this phenomenon and the transition rounding observed in simulations.
Area of Science:
- Materials Science
- Condensed Matter Physics
- Rheology
Background:
- Amorphous solids yield via a dynamical phase transition at a critical stress (Σc).
- Thermal fluctuations round this transition, enabling flow below Σc even in athermal systems.
- Understanding steady-state thermal flow in amorphous solids is crucial for predicting material behavior.
Purpose of the Study:
- To analytically solve thermally activated flow in amorphous solids at low temperatures using the Hébraud-Lequex (HL) model.
- To propose a general scaling law for transition rounding due to thermal fluctuations.
- To validate the proposed scaling law across different simulation models.
Main Methods:
- Mesoscopic elastoplastic modeling, specifically the Hébraud-Lequex (HL) model.
- Analytical solution for thermally activated flow at low temperatures.
- Numerical simulations including the HL model, a 2D elastoplastic model, and molecular dynamics of 2D Lennard-Jones glass.
Main Results:
- An analytical solution for thermally activated flow in the HL model at low temperatures was derived.
- A general scaling law was proposed, accurately describing the rounding of the yield transition.
- The scaling law demonstrated validity across various simulation approaches, confirming its broad applicability.
Conclusions:
- Thermal fluctuations significantly impact the yielding behavior of amorphous solids, leading to a rounded transition.
- The proposed general scaling law provides a unified framework for understanding this phenomenon.
- The findings are robust, confirmed by analytical solutions and diverse numerical simulations.
More Related Videos
Related Concept Videos
Viscosity
6.4K
When water is poured into a glass, it falls freely and quickly, whereas if honey or maple syrup is poured over a pancake, it flows slowly and sticks to the surface of the container. This difference in the flow of different kinds of liquids arises due to the fluid friction between the liquid layers and the liquid and the surrounding material. This property of fluids is called fluid viscosity. In this example, water has a lower viscosity than honey and maple syrup.
The SI unit of viscosity is...
The SI unit of viscosity is...
6.4K
Phase Transitions: Melting and Freezing
13.5K
Heating a crystalline solid increases the average energy of its atoms, molecules, or ions, and the solid gets hotter. At some point, the added energy becomes large enough to partially overcome the forces holding the molecules or ions of the solid in their fixed positions, and the solid begins the process of transitioning to the liquid state or melting. At this point, the temperature of the solid stops rising, despite the continual input of heat, and it remains constant until all of the solid is...
13.5K
Laminar and Turbulent Flow
9.5K
Fluid dynamics is the study of fluids in motion. Velocity vectors are often used to illustrate fluid motion in applications like meteorology. For example, wind—the fluid motion of air in the atmosphere—can be represented by vectors indicating the speed and direction of the wind at any given point on a map. Another method for representing fluid motion is a streamline. A streamline represents the path of a small volume of fluid as it flows. When the flow pattern changes with time, the...
9.5K
Couette Flow
542
Couette flow represents the flow of fluid between two parallel plates, with one plate fixed and the other moving with a constant velocity. This configuration allows for a simplified analysis using the Navier-Stokes equations, which govern fluid motion under conditions of viscosity and incompressibility. For Couette flow, the assumptions include a steady, laminar, incompressible flow with a zero-pressure gradient in the flow direction. This flow type is beneficial for understanding shear-driven...
542
Molecular and Ionic Solids
18.6K
Crystalline solids are divided into four types: molecular, ionic, metallic, and covalent network based on the type of constituent units and their interparticle interactions.
Molecular Solids
Molecular crystalline solids, such as ice, sucrose (table sugar), and iodine, are solids that are composed of neutral molecules as their constituent units. These molecules are held together by weak intermolecular forces such as London dispersion forces, dipole-dipole interactions, or hydrogen bonds, which...
Molecular Solids
Molecular crystalline solids, such as ice, sucrose (table sugar), and iodine, are solids that are composed of neutral molecules as their constituent units. These molecules are held together by weak intermolecular forces such as London dispersion forces, dipole-dipole interactions, or hydrogen bonds, which...
18.6K
Heating and Cooling Curves
24.9K
When a substance—isolated from its environment—is subjected to heat changes, corresponding changes in temperature and phase of the substance is observed; this is graphically represented by heating and cooling curves.
For instance, the addition of heat raises the temperature of a solid; the amount of heat absorbed depends on the heat capacity of the solid (q = mcsolidΔT). According to thermochemistry, the relation between the amount of heat absorbed or released by a substance, q, and its...
For instance, the addition of heat raises the temperature of a solid; the amount of heat absorbed depends on the heat capacity of the solid (q = mcsolidΔT). According to thermochemistry, the relation between the amount of heat absorbed or released by a substance, q, and its...
24.9K

