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Original Reports

A molecular dynamics study on the Mie-Grüneisen equation-of-state and high strain-rate behavior of equiatomic CoCrFeMnNi

, ORCID Icon & ORCID Icon
Pages 1055-1062 | Received 09 Aug 2023, Published online: 14 Nov 2023

Figures & data

Figure 1. (a) Points on the principle shock Hugoniot in Pρ space. The dashed red line only serves to indicate the trend of the data. (b) Points on the principle shock Hugoniot in UsUp space along with available experimental data. The solid red line represents the fitted analytic reference curve, Equation (Equation6).

Figure 1. (a) Points on the principle shock Hugoniot in P−ρ space. The dashed red line only serves to indicate the trend of the data. (b) Points on the principle shock Hugoniot in Us−Up space along with available experimental data. The solid red line represents the fitted analytic reference curve, Equation (Equation6(6) Us=2Cs[1−S1μ+(1−S1μ)2−4S2μ2]−1−Bexp⁡[−(μμ∗)N],(6) ).

Table 1. Calibrated Mie-Grüneisen EOS model parameters. The fitting parameter N was chosen to be fixed at 1.0.

Figure 2. Free surface velocity, ufs, traces for the NEMD simulations.

Figure 2. Free surface velocity, ufs, traces for the NEMD simulations.

Table 2. Strain-rate dependent spall strengths for CoCrFeMnNi calculated using Equation (Equation7).

Figure 3. Space-time-density diagrams showing the initial shock wave propagation and subsequent rarefaction waves along with the corresponding phase fraction evolution for (a) no spallation with u0=1.00 km/s and (b) spallation with u0=1.50 km/s.

Figure 3. Space-time-density diagrams showing the initial shock wave propagation and subsequent rarefaction waves along with the corresponding phase fraction evolution for (a) no spallation with u0=1.00 km/s and (b) spallation with u0=1.50 km/s.
Supplemental material

Supplemental Material

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Data availability

The data that support the findings of this study are available from the authors upon reasonable request.