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Heighway PG, Sliwa M, McGonegle D, Wehrenberg C, Bolme CA, Eggert J, Higginbotham A, Lazicki A, Lee HJ, Nagler B, Park HS, Rudd RE, Smith RF, Suggit MJ, Swift D, Tavella F, Remington BA, Wark JS. Nonisentropic Release of a Shocked Solid. PHYSICAL REVIEW LETTERS 2019; 123:245501. [PMID: 31922830 DOI: 10.1103/physrevlett.123.245501] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/18/2019] [Revised: 09/09/2019] [Indexed: 06/10/2023]
Abstract
We present molecular dynamics simulations of shock and release in micron-scale tantalum crystals that exhibit postbreakout temperatures far exceeding those expected under the standard assumption of isentropic release. We show via an energy-budget analysis that this is due to plastic-work heating from material strength that largely counters thermoelastic cooling. The simulations are corroborated by experiments where the release temperatures of laser-shocked tantalum foils are deduced from their thermal strains via in situ x-ray diffraction and are found to be close to those behind the shock.
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Affiliation(s)
- P G Heighway
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom
| | - M Sliwa
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom
| | - D McGonegle
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom
| | - C Wehrenberg
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94550, USA
| | - C A Bolme
- Los Alamos National Laboratory, Bikini Atoll Road, SM-30, Los Alamos, New Mexico 87545, USA
| | - J Eggert
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94550, USA
| | - A Higginbotham
- York Plasma Institute, University of York, Heslington, York YO10 5DD, United Kingdom
| | - A Lazicki
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94550, USA
| | - H J Lee
- SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA
| | - B Nagler
- SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA
| | - H-S Park
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94550, USA
| | - R E Rudd
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94550, USA
| | - R F Smith
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94550, USA
| | - M J Suggit
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom
| | - D Swift
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94550, USA
| | - F Tavella
- SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA
| | - B A Remington
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94550, USA
| | - J S Wark
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom
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E JC, Cai Y, Zhong ZY, Tang MX, Zhu XR, Wang L, Luo SN. Texture of nanocrystalline solids: atomic scale characterization and applications. J Appl Crystallogr 2018. [DOI: 10.1107/s1600576717018040] [Citation(s) in RCA: 6] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/10/2022] Open
Abstract
A methodology is presented to characterize the crystallographic texture of atomic configurations on the basis of Euler angles. Texture information characterized by orientation map, orientation distribution function, texture index, pole figure and inverse pole figure is obtained. The paper reports the construction and characterization of the texture of nanocrystalline configurations with different grain numbers, grain sizes and percentages of preferred orientation. The minimum grain number for texture-free configurations is ∼2500. The effect of texture on deducing grain size from simulated X-ray diffraction curves is also explored as an application case of texture analysis. In addition, molecular dynamics simulations are performed on initially texture-free nanocrystalline Ta under shock-wave loading, which shows a 〈001〉 + 〈111〉 double fiber texture after shock-wave compression.
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Park HS, Rudd RE, Cavallo RM, Barton NR, Arsenlis A, Belof JL, Blobaum KJM, El-dasher BS, Florando JN, Huntington CM, Maddox BR, May MJ, Plechaty C, Prisbrey ST, Remington BA, Wallace RJ, Wehrenberg CE, Wilson MJ, Comley AJ, Giraldez E, Nikroo A, Farrell M, Randall G, Gray GT. Grain-size-independent plastic flow at ultrahigh pressures and strain rates. PHYSICAL REVIEW LETTERS 2015; 114:065502. [PMID: 25723227 DOI: 10.1103/physrevlett.114.065502] [Citation(s) in RCA: 6] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/17/2014] [Indexed: 06/04/2023]
Abstract
A basic tenet of material science is that the flow stress of a metal increases as its grain size decreases, an effect described by the Hall-Petch relation. This relation is used extensively in material design to optimize the hardness, durability, survivability, and ductility of structural metals. This Letter reports experimental results in a new regime of high pressures and strain rates that challenge this basic tenet of mechanical metallurgy. We report measurements of the plastic flow of the model body-centered-cubic metal tantalum made under conditions of high pressure (>100 GPa) and strain rate (∼10(7) s(-1)) achieved by using the Omega laser. Under these unique plastic deformation ("flow") conditions, the effect of grain size is found to be negligible for grain sizes >0.25 μm sizes. A multiscale model of the plastic flow suggests that pressure and strain rate hardening dominate over the grain-size effects. Theoretical estimates, based on grain compatibility and geometrically necessary dislocations, corroborate this conclusion.
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Affiliation(s)
- H-S Park
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - R E Rudd
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - R M Cavallo
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - N R Barton
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - A Arsenlis
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - J L Belof
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - K J M Blobaum
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - B S El-dasher
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - J N Florando
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - C M Huntington
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - B R Maddox
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - M J May
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - C Plechaty
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - S T Prisbrey
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - B A Remington
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - R J Wallace
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - C E Wehrenberg
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - M J Wilson
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551, USA
| | - A J Comley
- Atomic Weapons Establishment, Aldermaston, Reading RG7 4PR, United Kingdom
| | - E Giraldez
- General Atomics, 3550 General Atomics Court, San Diego, California 92121, USA
| | - A Nikroo
- General Atomics, 3550 General Atomics Court, San Diego, California 92121, USA
| | - M Farrell
- General Atomics, 3550 General Atomics Court, San Diego, California 92121, USA
| | - G Randall
- General Atomics, 3550 General Atomics Court, San Diego, California 92121, USA
| | - G T Gray
- Los Alamos National Laboratory, P.O. Box 1663, Los Alamos, New Mexico 87545, USA
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Rudd RE, Arsenlis A, Barton NR, Cavallo RM, Comley AJ, Maddox BR, Marian J, Park HS, Prisbrey ST, Wehrenberg CE, Zepeda-Ruiz L, Remington BA. Multiscale strength (MS) models: their foundation, their successes, and their challenges. ACTA ACUST UNITED AC 2014. [DOI: 10.1088/1742-6596/500/11/112055] [Citation(s) in RCA: 14] [Impact Index Per Article: 1.4] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/12/2022]
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