2008
DOI: 10.1103/physrevb.77.174107
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Effects of theαεphase transition on wave propagation and spallation in laser shock-loaded iron

Abstract: Despite extensive research work on the ␣-phase transition occurring in shock-loaded iron, the kinetics of this transformation remain largely unknown. Here, we present time-resolved free surface velocity measurements in iron foils of thicknesses ranging from 150 to 520 m subjected to laser shocks of peak pressure of about 130 GPa and duration of about 3 ns. The records show an elastic precursor followed by a plastic front, but the double wave structure that is usually associated with the phase change does not a… Show more

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Cited by 44 publications
(22 citation statements)
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“…Then, this calculated ramp profile is used as boundary condition in the 1 D finite difference, Lagrangian hydro code SHYLAC [16,17] to simulate the dynamic response of iron, including the kinetics of the phase transition. The iron sample is discretized into cells of same mass, as recommended in Reference [18], of initial thickness about 0.01 µm.…”
Section: Numerical Simulationsmentioning
confidence: 99%
See 1 more Smart Citation
“…Then, this calculated ramp profile is used as boundary condition in the 1 D finite difference, Lagrangian hydro code SHYLAC [16,17] to simulate the dynamic response of iron, including the kinetics of the phase transition. The iron sample is discretized into cells of same mass, as recommended in Reference [18], of initial thickness about 0.01 µm.…”
Section: Numerical Simulationsmentioning
confidence: 99%
“…with the details of the equation of state for each pure phase described in the References [16,17]. The time evolution of the epsilon mass fraction X is governed by a kinetics law derived from the classical concept of nucleation and growth of phase [23][24][25] …”
Section: α − ε Kinetics Modelmentioning
confidence: 99%
“…Iron is a material of significant relevance for many research fields and applications, including the physics of the Earth's core, materials science, metallurgy, etc., and its behavior under shock conditions as well as its phase diagram at high pressures have been studied for decades [20][21][22][23][24][25]. The body-centered-cubic F e(α) to hexagonal-closed-packed F e(ǫ) phase transformation in particular has remained of interest to experimentalists and theorists alike ever since it was first reported in shock wave experiments almost fifty years ago [20].…”
mentioning
confidence: 99%
“…the region beneath the free surface should remain in the α phase, due to pressure decay below the 13 GPa threshold). This leads to drastic differences in the wave profiles, discussed in detail in [2]. The above model is shown to provide consistent velocity profiles with a time constant η set to 5 ns (Fig.…”
Section: -P2 New Models and Hydrocodes For Shock Wave Processesmentioning
confidence: 64%