Different universality classes at the yielding transition of amorphous systems
| Autor: | Eduardo Alberto Jagla |
|---|---|
| Rok vydání: | 2017 |
| Předmět: |
PLASTIC YIELDING
Physics Discrete mathematics Condensed Matter - Materials Science Mesoscopic physics Yield (engineering) Flow curve Statistical Mechanics (cond-mat.stat-mech) Ciencias Físicas Materials Science (cond-mat.mtrl-sci) FOS: Physical sciences Thermodynamics purl.org/becyt/ford/1.3 [https] Strain rate Critical value 01 natural sciences 010305 fluids & plasmas Amorphous solid Universality (dynamical systems) purl.org/becyt/ford/1 [https] Astronomía 0103 physical sciences 010306 general physics Condensed Matter - Statistical Mechanics CIENCIAS NATURALES Y EXACTAS |
| Zdroj: | CONICET Digital (CONICET) Consejo Nacional de Investigaciones Científicas y Técnicas instacron:CONICET |
| ISSN: | 2470-0053 2470-0045 |
| DOI: | 10.1103/physreve.96.023006 |
| Popis: | We study the yielding transition of a two dimensional amorphous system under shear by using a mesoscopic elasto-plastic model. The model combines a full (tensorial) description of the elastic interactions in the system, and the possibility of structural reaccommodations that are responsible for the plastic behavior. The possible structural reaccommodations are encoded in the form of a "plastic disorder" potential, which is chosen independently at each position of the sample to account for local heterogeneities. We observe that the stress must exceed a critical value $\sigma_c$ in order for the system to yield. In addition, when the system yields a flow curve relating stress $\sigma$ and strain rate $\dot\gamma$ of the form $\dot\gamma \sim(\sigma-\sigma_c)^\beta $ is obtained. Remarkably, we observe the value of $\beta$ to depend on some details of the plastic disorder potential. For smooth potentials a value of $\beta\simeq 2.0$ is obtained, whereas for potentials obtained as a concatenation of smooth pieces a value $\beta\simeq 1.5$ is observed in the simulations. This indicates a dependence of critical behavior on details of the plastic behavior that has not been pointed out before. In addition, by integrating out non-essential, harmonic degrees of freedom, we derive a simplified scalar version of the model that represents a collection of interacting Prandtl-Tomlinson particles. A mean field treatment of this interaction reproduces the difference of $\beta$ exponents for the two classes of plastic disorder potentials, and provides values of $\beta$ that compare favorably with those found in the full simulations. Comment: 13 pages, 12 figures |
| Databáze: | OpenAIRE |
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