4.6 Article

Unified crystal plasticity model for fcc metals: From quasistatic to shock loading

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PHYSICAL REVIEW B
卷 107, 期 2, 页码 -

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AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.107.024105

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The mechanical response of metals depends on the strain rate and shows significant changes across a wide range of strain rates. The authors developed a unified crystal plasticity model for face-centered cubic (fcc) metals to describe their mechanical response at different strain rates.
Mechanical response of metals is strongly dependent on the strain rate and exhibits drastic change as the strain rate varies across >10 orders of magnitude from quasistatic to shock loading. In this paper, we developed a unified crystal plasticity model for face-centered cubic (fcc) metals to describe the mechanical response in a wide range of strain rate from 10-5 to 107/s. The plasticity framework adopts the dislocation-based Orowan equation. Specifically, the mobility law for dislocation velocity incorporates both the thermal activation mech-anism dominating at low strain rates and drag mechanism dominating at high strain rates, through a repeating waiting-running model. The rate dependence of total dislocation density (rho t) evolution in the Orowan equation (implicitly) is captured by coupling the rate-dependent annihilation and the stress-dependent nucleation. More importantly, to capture the huge variation in mobile/total dislocation ratio (f = rho m/rho t) at different strain rates, we propose a physics-based law for mobile dislocation fraction f based on the exponential distribution of dislocation link lengths through a critical link length determined by the local stress. In addition, a thermohyperelastic model is supplemented to account for the nonlinear elastic behavior and thermoelastic coupling at shock loading. This unified model is validated against the mechanical response of single-crystal aluminum from quasistatic (10-5/s) to shock loading (107/s), where the features of thermal softening in static loading, thermal hardening in shock loading, and the strain-rate hardening in the medium strain-rate range are all quantitatively evaluated by a single set of parameters with a high average R2 value of 0.93.

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