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Published on: May 20, 2018
Long ranged stress correlations in the hard sphere liquid
Niklas Grimm1, Martin von Bischopinck2, Andreas Zumbusch2
1Fachbereich Physik, Universität Konstanz, 78457 Konstanz, Germany.
Shear elasticity emerges in glass-forming liquids, showing power-law stress correlations similar to solids. These correlations reveal spatial structures that grow with sound propagation, offering insights into the liquid-glass transition.
Area of Science:
- Condensed matter physics
- Materials science
- Statistical mechanics
Background:
- The liquid-to-glass transition is characterized by the emergence of shear elasticity.
- In solids, stresses around inclusions follow an Eshelby power law (r-D).
- Understanding stress dynamics in liquids is crucial for explaining glassy behavior.
Purpose of the Study:
- To investigate the emergence of Eshelby-like power-law stress correlations in glass-forming liquids.
- To analyze the spatial and temporal behavior of stress fields during the liquid-glass transition.
- To connect stress relaxation mechanisms to material properties like shear modulus and friction.
Main Methods:
- Molecular dynamics simulations of glass-forming hard sphere fluids.
- Detailed tensorial analysis of stress correlations.
- Examination of fluctuating force fields and shear stress dynamics.
Main Results:
- Observed unscreened power-law Eshelby patterns (r-D) in the stress correlations of the isotropic liquid state.
- Demonstrated that fluctuating force fields relax to zero, while shear stress correlations form power-law structures.
- Identified spatial regions where these structures grow with sound propagation, exhibiting exponents r-D and r-D-2.
- Showed that shear stresses relax diffusively within these regions in Brownian systems.
Conclusions:
- Glass-forming liquids exhibit solid-like stress correlation patterns prior to complete solidification.
- The emergence of these patterns is linked to sound propagation dynamics.
- Diffusive relaxation of shear stress is governed by shear modulus and friction in Brownian systems.
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