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LinearThermalExpansionCoeffCubic_fcc_Ni__TE_127978642829_001

Title
A single sentence description.
Linear thermal expansion coefficient of fcc Ni at 293.15 K under a pressure of 0 MPa v001
Description Linear thermal expansion coefficient of a fcc lattice of Ni atoms at a temperature of 293.15 K under a pressure of 0 MPa.
Species
The supported atomic species.
Ni
Disclaimer
A statement of applicability provided by the contributor, informing users of the intended use of this KIM Item.
None
Contributor Mwen
Maintainer Mwen
Author Mingjian Wen
Publication Year 2019
Item Citation

This Test is archived in OpenKIM [1-4].

[1] Wen M. Linear thermal expansion coefficient of fcc Ni at 293.15 K under a pressure of 0 MPa v001. OpenKIM; 2019.

[2] Wen M. Linear thermal expansion coefficient of cubic crystal structures v001. OpenKIM; 2019. doi:10.25950/fc69d82d

[3] Tadmor EB, Elliott RS, Sethna JP, Miller RE, Becker CA. The potential of atomistic simulations and the Knowledgebase of Interatomic Models. JOM. 2011;63(7):17. doi:10.1007/s11837-011-0102-6

[4] Elliott RS, Tadmor EB. Knowledgebase of Interatomic Models (KIM) Application Programming Interface (API). OpenKIM; 2011. doi:10.25950/ff8f563a

Click here to download the above citation in BibTeX format.
Short KIM ID
The unique KIM identifier code.
TE_127978642829_001
Extended KIM ID
The long form of the KIM ID including a human readable prefix (100 characters max), two underscores, and the Short KIM ID. Extended KIM IDs can only contain alpha-numeric characters (letters and digits) and underscores and must begin with a letter.
LinearThermalExpansionCoeffCubic_fcc_Ni__TE_127978642829_001
Citable Link https://openkim.org/cite/TE_127978642829_001
KIM Item TypeTest
DriverLinearThermalExpansionCoeffCubic__TD_522633393614_001
Properties
Properties as defined in kimspec.edn. These properties are inhereted from the Test Driver.
KIM API Version2.0
Simulator Name
The name of the simulator as defined in kimspec.edn. This Simulator Name is inhereted from the Test Driver.
LAMMPS
Programming Language(s)
The programming languages used in the code and the percentage of the code written in each one.
100.00% Python
Previous Version LinearThermalExpansionCoeffCubic_fcc_Ni__TE_127978642829_000


Models

EAM_Dynamo__MD_120291908751_005
Model Test Results Link to Test Results page Benchmark time
Usertime muliplied by the Whetstone Benchmark. This number can be used (approximately) to compare the performance of different models independently of the architecture on which the test was run.

Measured in Millions of Whetstone Instructions (MWI)
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EAM_Dynamo_AngeloMoodyBaskes_1995_NiAlH__MO_418978237058_005 view 9539760
EAM_Dynamo_BonnyCastinTerentyev_2013_FeNiCr__MO_763197941039_000 view 3612262
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EAM_Dynamo_BonnyPasianotMalerba_2009_FeNi__MO_267721408934_005 view 7688748
EAM_Dynamo_Foiles_1985_Ni__MO_010059867259_000 view 5522069
EAM_Dynamo_FoilesBaskesDaw_1986Universal3_Ni__MO_580571659842_000 view 4866007
EAM_Dynamo_MendelevKramerHao_2012_Ni__MO_832600236922_005 view 12006016
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EAM_Dynamo_Mishin_2004_NiAl__MO_101214310689_005 view 8338797
EAM_Dynamo_MishinFarkasMehl_1999_Ni__MO_400591584784_005 view 12735045
EAM_Dynamo_MishinMehlPapaconstantopoulos_2002_NiAl__MO_109933561507_005 view 16135252
EAM_Dynamo_OnatDurukanoglu_2014_CuNi__MO_592013496703_005 view 12997291
EAM_Dynamo_PunMishin_2009_NiAl__MO_751354403791_005 view 9109124
EAM_Dynamo_PunYamakovMishin_2013_NiAlCo__MO_826591359508_000 view 10083477
EAM_Dynamo_PunYamakovMishin_2015_NiCo__MO_010613863288_000 view 10119688
EAM_Dynamo_TehranchiCurtin_2010_NiH__MO_535504325462_003 view 9188136
EAM_Dynamo_WilsonMendelev_2015_NiZr__MO_306032198193_000 view 24303995
EAM_Dynamo_ZhangAshcraftMendelev_2016_NiNb__MO_047308317761_000 view 17647660
EAM_Dynamo_ZhouJohnsonWadley_2004_Ni__MO_110256178378_005 view 6534937
EAM_Dynamo_ZhouWadleyJohnson_2001NISTretabulation_Ni__MO_593762436933_000 view 7910784
EMT_Asap__MD_128315414717_004
Model Test Results Link to Test Results page Benchmark time
Usertime muliplied by the Whetstone Benchmark. This number can be used (approximately) to compare the performance of different models independently of the architecture on which the test was run.

Measured in Millions of Whetstone Instructions (MWI)
EMT_Asap_Standard_JacobsenStoltzeNorskov_1996_AlAgAuCuNiPdPt__MO_115316750986_001 view 25274029
EMT_Asap_Standard_JacobsenStoltzeNorskov_1996_Ni__MO_108408461881_001 view 15914272
Morse_Shifted__MD_552566534109_003
Model Test Results Link to Test Results page Benchmark time
Usertime muliplied by the Whetstone Benchmark. This number can be used (approximately) to compare the performance of different models independently of the architecture on which the test was run.

Measured in Millions of Whetstone Instructions (MWI)
Morse_Shifted_GirifalcoWeizer_1959HighCutoff_Ni__MO_381861218831_003 view 27630979
Morse_Shifted_GirifalcoWeizer_1959LowCutoff_Ni__MO_322509103239_003 view 7778829
Morse_Shifted_GirifalcoWeizer_1959MedCutoff_Ni__MO_758825945924_003 view 15538913
No Driver
Model Test Results Link to Test Results page Benchmark time
Usertime muliplied by the Whetstone Benchmark. This number can be used (approximately) to compare the performance of different models independently of the architecture on which the test was run.

Measured in Millions of Whetstone Instructions (MWI)
Sim_LAMMPS_ADP_MishinMehlPapaconstantopoulos_2005_Ni__SM_477692857359_000 view 8372353
Sim_LAMMPS_MEAM_AsadiZaeemNouranian_2015_Ni__SM_078420412697_000 view 37034337
Sim_LAMMPS_MEAM_KoGrabowskiNeugebauer_2015_NiTi__SM_770142935022_000 view 37889883
Sim_LAMMPS_MEAM_Wagner_2007_Ni__SM_168413969663_000 view 16598324





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