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LinearThermalExpansionCoeff_fcc_Ni__TE_127978642829_000

Title
A single sentence description.
Linear thermal expansion coefficient of fcc Ni at room temperature under zero pressure
Description This Test uses LAMMPS to compute the linear thermal expansion coefficient of fcc lattice Ni atoms at room temperature under zero pressure.
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 Mingjian Wen
Maintainer Mingjian Wen
Published on KIM 2015
How to Cite Click here to download this citation in BibTeX format.
Funding Not available
Short KIM ID
The unique KIM identifier code.
TE_127978642829_000
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.
LinearThermalExpansionCoeff_fcc_Ni__TE_127978642829_000
Citable Link https://openkim.org/cite/TE_127978642829_000
KIM Item TypeTest
DriverLinearThermalExpansionCoeffCubic__TD_522633393614_000
Properties
Properties as defined in kimspec.edn. These properties are inhereted from the Test Driver.
KIM API Version1.9.0
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


EAM_Dynamo__MD_120291908751_004
Model Test Results Link to Test Results page Benchmark time
Usertime multiplied 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)
EAM_Angelo_Moody_Baskes_modified_by_Tehranchi_Curtin_Song_Ni_H__MO_535504325462_002 view 5346923
EAM_Dynamo_Ackland_Tichy_Ni__MO_977363131043_004 view 3225201
EAM_Dynamo_Angelo_Moody_NiAlH__MO_418978237058_004 view 4800692
EAM_Dynamo_Bonny_Pasianot_FeCuNi__MO_469343973171_004 view 3942407
EAM_Dynamo_Bonny_Pasianot_FeNi__MO_267721408934_004 view 4045659
EAM_Dynamo_Mendelev_Ni__MO_832600236922_004 view 9126250
EAM_Dynamo_Mendelev_NiZr__MO_149104665840_004 view 13820136
EAM_Dynamo_Mishin_Farkas_Ni__MO_400591584784_004 view 12118675
EAM_Dynamo_Mishin_Mehl_NiAl__MO_109933561507_004 view 13871063
EAM_Dynamo_Mishin_NiAl__MO_101214310689_004 view 12161131
EAM_Dynamo_Onat_Durukanoglu_CuNi__MO_592013496703_004 view 7044436
EAM_Dynamo_PurjaPun_Mishin_NiAl__MO_751354403791_004 view 7289271
EAM_Dynamo_Zhou_Johnson_Ni__MO_110256178378_004 view 4353946
LennardJones612__MD_414112407348_002
Model Test Results Link to Test Results page Benchmark time
Usertime multiplied 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)
LennardJones612_UniversalShifted__MO_959249795837_002 view 13978550
Pair_Morse_Shifted__MD_552566534109_001
Model Test Results Link to Test Results page Benchmark time
Usertime multiplied 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)
Pair_Morse_Shifted_GirifalcoWeizer_HighCutoff_Ni__MO_381861218831_001 view 262591695
Pair_Morse_Shifted_GirifalcoWeizer_LowCutoff_Ni__MO_322509103239_001 view 50017188
Pair_Morse_Shifted_GirifalcoWeizer_MedCutoff_Ni__MO_758825945924_001 view 126531967





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LinearThermalExpansionCoeffCubic__TD_522633393614_000.zip Zip Windows archive
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