Relaxed energy as a function of tilt angle for a 110 symmetric tilt grain boundary in fcc Al v001

Brandon Runnels; Daniel S. Karls; Brendon Waters

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GrainBoundaryCubicCrystalSymmetricTiltRelaxedEnergyVsAngle_fcc110_Al__TE_202986963854_001

Title A single sentence description.	Relaxed energy as a function of tilt angle for a 110 symmetric tilt grain boundary in fcc Al v001
Description	Compute grain boundary energy relation for a Al 110 STGB
Species The supported atomic species.	Al
Disclaimer A statement of applicability provided by the contributor, informing users of the intended use of this KIM Item.	None

Contributor	Brandon Runnels
Maintainer	Brandon Runnels
Developer	Brandon Runnels Daniel S. Karls Brendon Waters
Published on KIM	2022
How to Cite	This Test is archived in OpenKIM [1-4]. [1] Runnels B, Karls DS, Waters B. Relaxed energy as a function of tilt angle for a 110 symmetric tilt grain boundary in fcc Al v001 [Internet]. OpenKIM; 2022. Available from: https://openkim.org/cite/TE_202986963854_001 [2] Runnels B, Karls DS, Waters B. Relaxed energy as a function of tilt angle for a symmetric tilt grain boundary within a cubic crystal v003. OpenKIM; 2022. doi:10.25950/2c59c9d6 [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.
Funding	Not available

Short KIM ID The unique KIM identifier code.	TE_202986963854_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.	GrainBoundaryCubicCrystalSymmetricTiltRelaxedEnergyVsAngle_fcc110_Al__TE_202986963854_001
Citable Link	https://openkim.org/cite/TE_202986963854_001
KIM Item Type	Test
Driver	GrainBoundaryCubicCrystalSymmetricTiltRelaxedEnergyVsAngle__TD_410381120771_003
Properties Properties as defined in kimspec.edn. These properties are inhereted from the Test Driver.	tag:brunnels@noreply.openkim.org,2016-02-18:property/grain-boundary-symmetric-tilt-energy-relaxed-relation-cubic-crystal
KIM API Version	2.2
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	GrainBoundaryCubicCrystalSymmetricTiltRelaxedEnergyVsAngle_fcc110_Al__TE_202986963854_000

Models

EAM_Dynamo__MD_120291908751_005

Model	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_Dynamo_AngeloMoodyBaskes_1995_NiAlH__MO_418978237058_005	view	11830528
EAM_Dynamo_CaiYe_1996_AlCu__MO_942551040047_005	view	33097834
EAM_Dynamo_FarkasCaro_2020_FeNiCrCoAl__MO_820335782779_000	view	16608965
EAM_Dynamo_FarkasJones_1996_NbTiAl__MO_042691367780_000	view	22580692
EAM_Dynamo_LandaWynblattSiegel_2000_AlPb__MO_699137396381_005	view	13700376
EAM_Dynamo_LiuAdams_1998_AlMg__MO_019873715786_000	view	19639193
EAM_Dynamo_LiuLiuBorucki_1999_AlCu__MO_020851069572_000	view	33719829
EAM_Dynamo_MendelevAstaRahman_2009_AlMg__MO_658278549784_005	view	22873861
EAM_Dynamo_MendelevFangYe_2015_AlSm__MO_338600200739_000	view	76754491
EAM_Dynamo_MendelevKramerBecker_2008_Al__MO_106969701023_005	view	45248171
EAM_Dynamo_MendelevSrolovitzAckland_2005_AlFe__MO_577453891941_005	view	18942724
EAM_Dynamo_Mishin_2004_NiAl__MO_101214310689_005	view	32036514
EAM_Dynamo_MishinFarkasMehl_1999_Al__MO_651801486679_005	view	15779548
EAM_Dynamo_MishinMehlPapaconstantopoulos_2002_NiAl__MO_109933561507_005 This Model has a disclaimer This potential was developed to accurately reproduce properties of a single phase of the Ni-Al system, namely, B2-NiAl. Properties of other phases of this system are reproduced less accurately. Application of this particular potential to simulations of pure Ni or pure Al is not recommended.	view	47963958
EAM_Dynamo_PunMishin_2009_NiAl__MO_751354403791_005 This Model has a disclaimer The paper reporting on this potential (G.P. Purja Pun and Y. Mishin, "Development of an interatomic potential for the Ni-Al system," Phil. Mag. 89, 3245 (2009)) contains an error in Table 6. The generalized stacking fault energies in Ni3Al listed in this table are incorrect. The correct energies computed with the new potential are (in J/m2): APB (111) 180 CSF (111) 229 SISF (111) 21 APB (100) 20	view	16199687
EAM_Dynamo_PunYamakovMishin_2013_AlCo__MO_678952612413_000	view	19644514
EAM_Dynamo_PunYamakovMishin_2013_NiAlCo__MO_826591359508_000	view	20308091
EAM_Dynamo_SongMendelev_2021_AlSm__MO_722733117926_000	view	50959471
EAM_Dynamo_SturgeonLaird_2000_Al__MO_120808805541_005 This Model has a disclaimer This model was developed as a prototype case for the Gibbs-Duhem protocol for optimizing melting points. As such, the melting point was the primary metric for its development. We have shown that the modifications to the original Mei-Davenport potential that we used to optimize T_m did not change the quality of the potential with respect to elastic constants, density, etc., but no systematic study of other properties was performed.	view	22046463
EAM_Dynamo_VailheFarkas_1997_CoAl__MO_284963179498_005	view	13355449
EAM_Dynamo_WineyKubotaGupta_2010_Al__MO_149316865608_005 This Model has a disclaimer Model was fit to room temperature properties and extrapolated, classical (i.e. non-quantum) low temperature properties. The intended application is for shock compression simulations, but validation against shock pressure conditions is limited. The model appears to provide accurate results in the elastic shock regime (i.e. pressure ~ 5 to 10 GPa), as documented in the paper by Zimmerman, Winey and Gupta (Phys. Rev. B, 2011). Behavior at higher pressures and in the elastic-plastic regime is unknown.	view	19674620
EAM_Dynamo_Zhakhovsky_2009_Al__MO_519613893196_000	view	33844318
EAM_Dynamo_ZhouJohnsonWadley_2004_Al__MO_131650261510_005	view	27689853
EAM_Dynamo_ZhouJohnsonWadley_2004_CuAgAuNiPdPtAlPbFeMoTaWMgCoTiZr__MO_870117231765_000	view	43942530
EAM_Dynamo_ZhouJohnsonWadley_2004NISTretabulation_Al__MO_060567868558_000	view	27756458
EAM_Dynamo_ZhouWadleyJohnson_2001_Al__MO_049243498555_000	view	77875073
EAM_Dynamo_ZopeMishin_2003_Al__MO_664470114311_005	view	19284021
EAM_Dynamo_ZopeMishin_2003_TiAl__MO_117656786760_005	view	32434914

EAM_IMD__MD_113599595631_003

Model	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_IMD_BrommerGaehler_2006A_AlNiCo__MO_122703700223_003	view	32711519
EAM_IMD_BrommerGaehler_2006B_AlNiCo__MO_128037485276_003	view	25934344
EAM_IMD_SchopfBrommerFrigan_2012_AlMnPd__MO_878712978062_003	view	71306442

EMT_Asap__MD_128315414717_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)
EMT_Asap_Standard_JacobsenStoltzeNorskov_1996_Al__MO_623376124862_001		view	24268578
EMT_Asap_Standard_JacobsenStoltzeNorskov_1996_AlAgAuCuNiPdPt__MO_115316750986_001		view	25299222

MEAM_LAMMPS__MD_249792265679_001

Model	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)
MEAM_LAMMPS_AlmyrasSangiovanniSarakinos_2019_NAlTi__MO_958395190627_001	view	138596156
MEAM_LAMMPS_DickelBaskesAslam_2018_MgAlZn__MO_093637366498_001	view	220649196
MEAM_LAMMPS_DongKimKo_2012_CoAl__MO_099716416216_001	view	103165243
MEAM_LAMMPS_JelinekGrohHorstemeyer_2012_AlSiMgCuFe__MO_262519520678_001	view	155838593
MEAM_LAMMPS_KimKimJung_2017_NiAlTi__MO_478967255435_001	view	147948781
MEAM_LAMMPS_KimKimLee_2009_AlMg__MO_058537087384_001	view	147175313
MEAM_LAMMPS_KimSeolJi_2017_PtAl__MO_793141037706_001	view	215781697
MEAM_LAMMPS_ShimKoKim_2013_AlVH__MO_344724145339_001	view	147731187

MEAM_LAMMPS__MD_249792265679_002

Model	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)
MEAM_LAMMPS_CostaAgrenClavaguera_2007_AlNi__MO_131642768288_002	view	66393121
MEAM_LAMMPS_JeongParkDo_2018_PdAl__MO_616482358807_002	view	67519644
MEAM_LAMMPS_KimJungLee_2015_NiAlCo__MO_876687166519_002	view	67568579
MEAM_LAMMPS_KimKimJung_2016_AlTi__MO_618133763375_002	view	69186872
MEAM_LAMMPS_KoShimLee_2011_AlH__MO_127847080751_002	view	68538075
MEAM_LAMMPS_LeeLee_2010_FeAl__MO_332211522050_002	view	20158294
MEAM_LAMMPS_LeeShimBaskes_2003_Al__MO_353977746962_001	view	66466582
MEAM_LAMMPS_MahataMukhopadhyayAsleZaeem_2022_AlFe__MO_304347095149_001	view	51014854
MEAM_LAMMPS_MahataMukhopadhyayAsleZaeem_2022_AlNi__MO_461927113651_001	view	56603283
MEAM_LAMMPS_PascuetFernandez_2015_Al__MO_315820974149_002	view	69880298
MEAM_LAMMPS_PascuetFernandez_2015_AlU__MO_596300673917_002	view	70219924
MEAM_LAMMPS_RoyDuttaChakraborti_2021_AlLi__MO_971738391444_001	view	72451617
MEAM_LAMMPS_SunRamachandranWick_2018_TiAl__MO_022920256108_002	view	26895774

Morse_Shifted__MD_552566534109_004

Model	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)
Morse_Shifted_GirifalcoWeizer_1959HighCutoff_Al__MO_140175748626_004	view	136356668
Morse_Shifted_GirifalcoWeizer_1959LowCutoff_Al__MO_411898953661_004	view	36321370
Morse_Shifted_GirifalcoWeizer_1959MedCutoff_Al__MO_279544746097_004	view	81039615

Tersoff_LAMMPS__MD_077075034781_005

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)
Tersoff_LAMMPS_PlummerRathodSrivastava_2021_TiAlC__MO_992900971352_000		view	257506844
Tersoff_LAMMPS_PlummerTucker_2019_TiAlC__MO_736419017411_000		view	257366813

No Driver

Model	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_ErcolessiAdams_1994_Al__MO_324507536345_003	view	31240160
Sim_LAMMPS_ADP_ApostolMishin_2011_AlCu__SM_667696763561_000	view	32678971
Sim_LAMMPS_ADP_StarikovGordeevLysogorskiy_2020_SiAuAl__SM_113843830602_000	view	29419200

Errors

EAM_CubicNaturalSpline__MD_853402641673_002

Model	Error Categories	Link to Error page
EAM_CubicNaturalSpline_ErcolessiAdams_1994_Al__MO_800509458712_002	other	view

EAM_Dynamo__MD_120291908751_005

Model	Error Categories	Link to Error page
EAM_Dynamo_ErcolessiAdams_1994_Al__MO_123629422045_005	other	view
EAM_Dynamo_JacobsenNorskovPuska_1987_Al__MO_411692133366_000	other	view
EAM_Dynamo_SchopfBrommerFrigan_2012_AlMnPd__MO_137572817842_000	other	view

EAM_QuinticClampedSpline__MD_532469991695_003

Model	Error Categories	Link to Error page
EAM_QuinticClampedSpline_ErcolessiAdams_1994_Al__MO_450093727396_002	other	view

EAM_QuinticHermiteSpline__MD_029719603993_003

Model	Error Categories	Link to Error page
EAM_QuinticHermiteSpline_ErcolessiAdams_1994_Al__MO_781138671863_002	other	view

LJ__MD_414112407348_003

Model	Error Categories	Link to Error page
LJ_ElliottAkerson_2015_Universal__MO_959249795837_003	other	view

MEAM_LAMMPS__MD_249792265679_002

Model	Error Categories	Link to Error page
MEAM_LAMMPS_AlmyrasSangiovanniSarakinos_2019_NAlTi__MO_958395190627_002	other	view
MEAM_LAMMPS_DickelBaskesAslam_2018_MgAlZn__MO_093637366498_002	other	view
MEAM_LAMMPS_DongKimKo_2012_CoAl__MO_099716416216_002	other	view
MEAM_LAMMPS_JelinekGrohHorstemeyer_2012_AlSiMgCuFe__MO_262519520678_002	other	view
MEAM_LAMMPS_KimKimJung_2017_NiAlTi__MO_478967255435_002	other	view
MEAM_LAMMPS_KimKimLee_2009_AlMg__MO_058537087384_002	other	view
MEAM_LAMMPS_KimSeolJi_2017_PtAl__MO_793141037706_002	other	view
MEAM_LAMMPS_ShimKoKim_2013_AlVH__MO_344724145339_002	other	view

Files

LICENSE
LICENSE.CDDL
Makefile
README.txt
dependencies.edn
kimprovenance.edn
kimspec.edn
pipeline.stdin.tpl
runner

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GrainBoundaryCubicCrystalSymmetricTiltRelaxedEnergyVsAngle_fcc110_Al__TE_202986963854_001.txz	Tar+XZ	Linux and OS X archive
GrainBoundaryCubicCrystalSymmetricTiltRelaxedEnergyVsAngle_fcc110_Al__TE_202986963854_001.zip	Zip	Windows archive

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This Test requires a Test Driver. Archives for the Test Driver GrainBoundaryCubicCrystalSymmetricTiltRelaxedEnergyVsAngle__TD_410381120771_003 appear below.

GrainBoundaryCubicCrystalSymmetricTiltRelaxedEnergyVsAngle__TD_410381120771_003.txz	Tar+XZ	Linux and OS X archive
GrainBoundaryCubicCrystalSymmetricTiltRelaxedEnergyVsAngle__TD_410381120771_003.zip	Zip	Windows archive

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