Abstract
The dynamic strength for a broad range of materials with different microstructures exhibits surprisingly similar behavior. Two distinct regimes are observed with a sharp transition between them. At low loading rates, the strength has a weak linear dependence on the log loading rate until a critical rate above which a dramatic increase is observed. We explain this behavior by considering material failure as a bond-breaking process driven by external loading and thermal fluctuation within a Langevin dynamics framework. The analysis leads to nondimensional measures for which the dynamic response collapses onto a universal curve, independent of material properties, describing both loading rate regimes and the transition between them. A simple approximate model is derived that provides an excellent fit to experimental data for a broad range of materials, including concrete, ceramics, and metals.
Original language | English (US) |
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Article number | 104715 |
Journal | Journal of the Mechanics and Physics of Solids |
Volume | 159 |
DOIs | |
State | Published - Feb 2022 |
Externally published | Yes |
Bibliographical note
Publisher Copyright:© 2021 Elsevier Ltd
Keywords
- Damped dynamics
- Dynamic fracture
- Dynamic increase factor
- Dynamic material strength
- Fiber bundle model
- Fokker–Planck equation
- Langevin equation
- Nonequilibrium statistical physics
- Reaction rate theory