cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1708563
title: Materials Data on ZrIn2O5 by Materials Project

description: ZrO2In2O3 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Zr4+ is bonded to six O2- atoms to form distorted ZrO6 octahedra that share corners with two equivalent ZrO6 octahedra, corners with eight InO6 octahedra, and edges with two equivalent ZrO6 octahedra. The corner-sharing octahedra tilt angles range from 40–69°. There are a spread of Zr–O bond distances ranging from 1.97–2.32 Å. There are two inequivalent In3+ sites. In the first In3+ site, In3+ is bonded to six O2- atoms to form distorted InO6 octahedra that share corners with two equivalent InO6 octahedra, corners with four equivalent ZrO6 octahedra, and edges with six InO6 octahedra. The corner-sharing octahedra tilt angles range from 56–69°. There are a spread of In–O bond distances ranging from 2.21–2.35 Å. In the second In3+ site, In3+ is bonded to six O2- atoms to form InO6 octahedra that share corners with four equivalent ZrO6 octahedra, corners with four InO6 octahedra, and edges with four InO6 octahedra. The corner-sharing octahedra tilt angles range from 56–66°. There are a spread of In–O bond distances ranging from 2.21–2.35 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to one Zr4+ and two equivalent In3+ atoms. In the second O2- site, O2- is bonded to one Zr4+ and three equivalent In3+ atoms to form a mixture of edge and corner-sharing OZrIn3 tetrahedra. In the third O2- site, O2- is bonded to one Zr4+ and three In3+ atoms to form distorted OZrIn3 tetrahedra that share corners with eight OZrIn3 tetrahedra and edges with two equivalent OIn4 tetrahedra. In the fourth O2- site, O2- is bonded to four In3+ atoms to form OIn4 tetrahedra that share corners with ten OIn4 tetrahedra and edges with three OZrIn3 tetrahedra. In the fifth O2- site, O2- is bonded in a 3-coordinate geometry to three equivalent Zr4+ atoms.
DOI: 10.17188/1708564
title: Materials Data on InS2 by Materials Project

description: InS2 crystallizes in the tetragonal P4/nmm space group. The structure is three-dimensional. In3+ is bonded in a 4-coordinate geometry to nine S+1.50- atoms. There are a spread of In–S bond distances ranging from 2.67–3.22 Å. There are two inequivalent S+1.50- sites. In the first S+1.50- site, S+1.50- is bonded in a 5-coordinate geometry to five equivalent In3+ atoms. In the second S+1.50- site, S+1.50- is bonded to four equivalent In3+ and four equivalent S+1.50- atoms to form a mixture of distorted corner, edge, and face-sharing SIn4S4 hexagonal bipyramids. All S–S bond lengths are 2.58 Å.
DOI: 10.17188/1708566
title: Materials Data on Pr2Mo4O15 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1708567
title: Materials Data on Ba2SmV3O11 by Materials Project

description: Ba2SmV3O11 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Ba–O bond distances ranging from 2.75–3.39 Å. In the second Ba2+ site, Ba2+ is bonded in a 11-coordinate geometry to eleven O2- atoms. There are a spread of Ba–O bond distances ranging from 2.81–3.16 Å. Sm3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Sm–O bond distances ranging from 2.31–2.86 Å. There are three inequivalent V5+ sites. In the first V5+ site, V5+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of V–O bond distances ranging from 1.70–1.78 Å. In the second V5+ site, V5+ is bonded to four O2- atoms to form corner-sharing VO4 tetrahedra. There are a spread of V–O bond distances ranging from 1.70–1.82 Å. In the third V5+ site, V5+ is bonded to four O2- atoms to form corner-sharing VO4 tetrahedra. There are a spread of V–O bond distances ranging from 1.70–1.83 Å. There are eleven inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted linear geometry to two equivalent Ba2+ and two V5+ atoms. In the second O2- site, O2- is bonded in a distorted single-bond geometry to three Ba2+ and one V5+ atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to three Ba2+ and one V5+ atom. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to three Ba2+ and one V5+ atom. In the fifth O2- site, O2- is bonded in a 1-coordinate geometry to one Ba2+, two equivalent Sm3+, and one V5+ atom. In the sixth O2- site, O2- is bonded in a distorted single-bond geometry to three Ba2+ and one V5+ atom. In the seventh O2- site, O2- is bonded in a distorted single-bond geometry to one Ba2+, two equivalent Sm3+, and one V5+ atom. In the eighth O2- site, O2- is bonded in a distorted single-bond geometry to two Ba2+ and one V5+ atom. In the ninth O2- site, O2- is bonded in a 2-coordinate geometry to one Ba2+, one Sm3+, and one V5+ atom. In the tenth O2- site, O2- is bonded in a 3-coordinate geometry to one Ba2+, two equivalent Sm3+, and one V5+ atom. In the eleventh O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Ba2+, one Sm3+, and one V5+ atom.
DOI: 10.17188/1708568
title: Materials Data on Al(MoS2)12 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1708569
title: Materials Data on KTm(MoO4)2 by Materials Project

description: KTm(MoO4)2 crystallizes in the orthorhombic Pbcn space group. The structure is three-dimensional. K1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of K–O bond distances ranging from 2.72–2.89 Å. Tm3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Tm–O bond distances ranging from 2.26–2.52 Å. Mo6+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of Mo–O bond distances ranging from 1.76–1.87 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Tm3+ and one Mo6+ atom. In the second O2- site, O2- is bonded in a 2-coordinate geometry to one K1+, one Tm3+, and one Mo6+ atom. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent K1+ and one Mo6+ atom. In the fourth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Tm3+ and one Mo6+ atom.
DOI: 10.17188/1708572
title: Materials Data on CeAlIr by Materials Project

description: CeIrAl crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Ce is bonded to six equivalent Ir and six equivalent Al atoms to form a mixture of face and edge-sharing CeAl6Ir6 cuboctahedra. All Ce–Ir bond lengths are 3.10 Å. All Ce–Al bond lengths are 3.10 Å. Ir is bonded in a 3-coordinate geometry to six equivalent Ce and three equivalent Al atoms. All Ir–Al bond lengths are 2.57 Å. Al is bonded in a distorted trigonal planar geometry to six equivalent Ce and three equivalent Ir atoms.
DOI: 10.17188/1708573
title: Materials Data on Tb3Sc by Materials Project

description: Tb3Sc is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Tb is bonded to eight equivalent Tb and four equivalent Sc atoms to form TbTb8Sc4 cuboctahedra that share corners with twelve equivalent TbTb8Sc4 cuboctahedra, edges with eight equivalent ScTb12 cuboctahedra, edges with sixteen equivalent TbTb8Sc4 cuboctahedra, faces with four equivalent ScTb12 cuboctahedra, and faces with fourteen equivalent TbTb8Sc4 cuboctahedra. All Tb–Tb bond lengths are 3.49 Å. All Tb–Sc bond lengths are 3.49 Å. Sc is bonded to twelve equivalent Tb atoms to form ScTb12 cuboctahedra that share corners with twelve equivalent ScTb12 cuboctahedra, edges with twenty-four equivalent TbTb8Sc4 cuboctahedra, faces with six equivalent ScTb12 cuboctahedra, and faces with twelve equivalent TbTb8Sc4 cuboctahedra.
DOI: 10.17188/1708574
title: Materials Data on RbSeO4 by Materials Project

description: RbSeO4 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are three inequivalent Rb sites. In the first Rb site, Rb is bonded in a 10-coordinate geometry to ten O atoms. There are a spread of Rb–O bond distances ranging from 2.86–3.33 Å. In the second Rb site, Rb is bonded in a 10-coordinate geometry to ten O atoms. There are a spread of Rb–O bond distances ranging from 2.90–3.54 Å. In the third Rb site, Rb is bonded in a 10-coordinate geometry to ten O atoms. There are a spread of Rb–O bond distances ranging from 2.88–3.53 Å. There are three inequivalent Se sites. In the first Se site, Se is bonded in a tetrahedral geometry to four O atoms. There is two shorter (1.65 Å) and two longer (1.72 Å) Se–O bond length. In the second Se site, Se is bonded in a tetrahedral geometry to four O atoms. There are a spread of Se–O bond distances ranging from 1.65–1.72 Å. In the third Se site, Se is bonded in a tetrahedral geometry to four O atoms. There is two shorter (1.65 Å) and two longer (1.72 Å) Se–O bond length. There are twelve inequivalent O sites. In the first O site, O is bonded in a distorted single-bond geometry to two Rb and one Se atom. In the second O site, O is bonded in a 1-coordinate geometry to three Rb and one Se atom. In the third O site, O is bonded in a distorted single-bond geometry to two Rb and one Se atom. In the fourth O site, O is bonded in a 1-coordinate geometry to three Rb and one Se atom. In the fifth O site, O is bonded in a single-bond geometry to two Rb and one Se atom. In the sixth O site, O is bonded in a 4-coordinate geometry to three Rb and one Se atom. In the seventh O site, O is bonded in a 1-coordinate geometry to three Rb and one Se atom. In the eighth O site, O is bonded in a distorted single-bond geometry to two Rb and one Se atom. In the ninth O site, O is bonded in a distorted single-bond geometry to two Rb and one Se atom. In the tenth O site, O is bonded in a 1-coordinate geometry to three Rb and one Se atom. In the eleventh O site, O is bonded in a distorted single-bond geometry to two Rb and one Se atom. In the twelfth O site, O is bonded in a 1-coordinate geometry to three Rb and one Se atom.
DOI: 10.17188/1708575
title: Materials Data on Co(CN)2 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1708576
title: Materials Data on NbVH4 by Materials Project

description: NbVH4 is Fluorite-derived structured and crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Nb2+ is bonded in a body-centered cubic geometry to eight equivalent H1- atoms. All Nb–H bond lengths are 1.97 Å. V2+ is bonded in a body-centered cubic geometry to eight equivalent H1- atoms. All V–H bond lengths are 1.85 Å. H1- is bonded to two equivalent Nb2+ and two equivalent V2+ atoms to form a mixture of edge and corner-sharing HNb2V2 tetrahedra.
DOI: 10.17188/1708577
title: Materials Data on Mg2In3MoS8 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1708578
title: Materials Data on EuCuGe by Materials Project

description: EuCuGe crystallizes in the orthorhombic Pna2_1 space group. The structure is three-dimensional. there are three inequivalent Eu sites. In the first Eu site, Eu is bonded in a 12-coordinate geometry to six Cu and six Ge atoms. There are a spread of Eu–Cu bond distances ranging from 3.08–3.33 Å. There are a spread of Eu–Ge bond distances ranging from 3.13–3.35 Å. In the second Eu site, Eu is bonded in a 12-coordinate geometry to six Cu and six Ge atoms. There are a spread of Eu–Cu bond distances ranging from 3.27–3.36 Å. There are a spread of Eu–Ge bond distances ranging from 3.10–3.22 Å. In the third Eu site, Eu is bonded in a 12-coordinate geometry to six Cu and six Ge atoms. There are a spread of Eu–Cu bond distances ranging from 3.13–3.18 Å. There are a spread of Eu–Ge bond distances ranging from 3.20–3.38 Å. There are three inequivalent Cu sites. In the first Cu site, Cu is bonded in a 10-coordinate geometry to six Eu, one Cu, and three Ge atoms. The Cu–Cu bond length is 3.11 Å. There are a spread of Cu–Ge bond distances ranging from 2.56–2.60 Å. In the second Cu site, Cu is bonded in a 10-coordinate geometry to six Eu, one Cu, and three equivalent Ge atoms. There are a spread of Cu–Ge bond distances ranging from 2.59–2.65 Å. In the third Cu site, Cu is bonded in a 10-coordinate geometry to six Eu and four Ge atoms. There are a spread of Cu–Ge bond distances ranging from 2.61–2.99 Å. There are three inequivalent Ge sites. In the first Ge site, Ge is bonded in a 10-coordinate geometry to six Eu, three Cu, and one Ge atom. The Ge–Ge bond length is 2.85 Å. In the second Ge site, Ge is bonded in a 10-coordinate geometry to six Eu, three equivalent Cu, and one Ge atom. In the third Ge site, Ge is bonded in a 10-coordinate geometry to six Eu and four Cu atoms.
DOI: 10.17188/1708579
title: Materials Data on Na4Ce2(Si4O11)3 by Materials Project

description: (Na2Ce(Si3O8)2)4O2 crystallizes in the orthorhombic Pmm2 space group. The structure is three-dimensional and consists of one water molecule and one Na2Ce(Si3O8)2 framework. In the Na2Ce(Si3O8)2 framework, there are two inequivalent Na sites. In the first Na site, Na is bonded in a 6-coordinate geometry to six O atoms. There are a spread of Na–O bond distances ranging from 2.30–2.81 Å. In the second Na site, Na is bonded to five O atoms to form distorted NaO5 trigonal bipyramids that share corners with four SiO4 tetrahedra and edges with two equivalent NaO5 trigonal bipyramids. There are a spread of Na–O bond distances ranging from 2.42–2.73 Å. Ce is bonded in a 7-coordinate geometry to seven O atoms. There are a spread of Ce–O bond distances ranging from 2.18–2.76 Å. There are four inequivalent Si sites. In the first Si site, Si is bonded to four O atoms to form corner-sharing SiO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.62–1.64 Å. In the second Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share corners with three SiO4 tetrahedra and a cornercorner with one NaO5 trigonal bipyramid. There are a spread of Si–O bond distances ranging from 1.62–1.65 Å. In the third Si site, Si is bonded to four O atoms to form corner-sharing SiO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.60–1.67 Å. In the fourth Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share corners with three SiO4 tetrahedra and corners with two equivalent NaO5 trigonal bipyramids. There are a spread of Si–O bond distances ranging from 1.61–1.64 Å. There are twelve inequivalent O sites. In the first O site, O is bonded in a bent 150 degrees geometry to two Si atoms. In the second O site, O is bonded in a distorted trigonal planar geometry to one Na and two equivalent Si atoms. In the third O site, O is bonded in a distorted linear geometry to one Ce and one Si atom. In the fourth O site, O is bonded in a distorted bent 150 degrees geometry to one Ce and two Si atoms. In the fifth O site, O is bonded to two equivalent Na, one Ce, and one Si atom to form distorted edge-sharing ONa2CeSi tetrahedra. In the sixth O site, O is bonded in a bent 150 degrees geometry to one Na and two equivalent Si atoms. In the seventh O site, O is bonded in a bent 150 degrees geometry to two equivalent Si atoms. In the eighth O site, O is bonded in a distorted trigonal planar geometry to three Na atoms. In the ninth O site, O is bonded in a bent 150 degrees geometry to two equivalent Si atoms. In the tenth O site, O is bonded in a 1-coordinate geometry to one Na, one Ce, and one Si atom. In the eleventh O site, O is bonded in a 3-coordinate geometry to one Na, one Ce, and one Si atom. In the twelfth O site, O is bonded in a distorted bent 120 degrees geometry to two Si atoms.
DOI: 10.17188/1708580
title: Materials Data on Pb4SeS3 by Materials Project

description: Pb4SeS3 is Caswellsilverite-like structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. there are two inequivalent Pb2+ sites. In the first Pb2+ site, Pb2+ is bonded to six S2- atoms to form a mixture of edge and corner-sharing PbS6 octahedra. The corner-sharing octahedra tilt angles range from 0–1°. All Pb–S bond lengths are 3.02 Å. In the second Pb2+ site, Pb2+ is bonded to three equivalent Se2- and three equivalent S2- atoms to form a mixture of edge and corner-sharing PbSe3S3 octahedra. The corner-sharing octahedra tilt angles range from 0–1°. All Pb–Se bond lengths are 3.07 Å. All Pb–S bond lengths are 2.99 Å. Se2- is bonded to six equivalent Pb2+ atoms to form SePb6 octahedra that share corners with six equivalent SPb6 octahedra, edges with six equivalent SePb6 octahedra, and edges with six equivalent SPb6 octahedra. The corner-sharing octahedral tilt angles are 2°. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded to six Pb2+ atoms to form SPb6 octahedra that share corners with three equivalent SePb6 octahedra, corners with three equivalent SPb6 octahedra, edges with three equivalent SePb6 octahedra, and edges with nine SPb6 octahedra. The corner-sharing octahedra tilt angles range from 0–2°. In the second S2- site, S2- is bonded to six equivalent Pb2+ atoms to form a mixture of edge and corner-sharing SPb6 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1708581
title: Materials Data on Si2Ge5N6 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1708582
title: Materials Data on LiEuF2 by Materials Project

description: LiEuF2 crystallizes in the tetragonal I4_1/a space group. The structure is three-dimensional. Li is bonded in a square co-planar geometry to four equivalent F atoms. There are two shorter (2.32 Å) and two longer (2.34 Å) Li–F bond lengths. Eu is bonded to six equivalent F atoms to form edge-sharing EuF6 octahedra. There are a spread of Eu–F bond distances ranging from 2.51–2.54 Å. F is bonded to two equivalent Li and three equivalent Eu atoms to form a mixture of distorted edge and corner-sharing FLi2Eu3 trigonal bipyramids.
DOI: 10.17188/1708583
title: Materials Data on Mn3Pt by Materials Project

description: Mn3Pt is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Mn is bonded in a 12-coordinate geometry to four equivalent Pt atoms. There are two shorter (2.61 Å) and two longer (2.62 Å) Mn–Pt bond lengths. Pt is bonded to twelve equivalent Mn atoms to form a mixture of corner and face-sharing PtMn12 cuboctahedra.
DOI: 10.17188/1708584
title: Materials Data on Pr3Sb4Pt7 by Materials Project

description: Pr3Pt7Sb4 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Pr3+ sites. In the first Pr3+ site, Pr3+ is bonded in a 8-coordinate geometry to eight Pt+1.43- atoms. There are a spread of Pr–Pt bond distances ranging from 3.11–3.32 Å. In the second Pr3+ site, Pr3+ is bonded in a 2-coordinate geometry to ten Pt+1.43- atoms. There are a spread of Pr–Pt bond distances ranging from 3.20–3.62 Å. There are four inequivalent Pt+1.43- sites. In the first Pt+1.43- site, Pt+1.43- is bonded in a 10-coordinate geometry to four Pr3+, one Pt+1.43-, and four Sb+0.25+ atoms. The Pt–Pt bond length is 2.87 Å. There are a spread of Pt–Sb bond distances ranging from 2.65–2.78 Å. In the second Pt+1.43- site, Pt+1.43- is bonded in a 12-coordinate geometry to four Pr3+, five Pt+1.43-, and three Sb+0.25+ atoms. There are two shorter (2.85 Å) and two longer (3.16 Å) Pt–Pt bond lengths. There are two shorter (2.77 Å) and one longer (2.78 Å) Pt–Sb bond lengths. In the third Pt+1.43- site, Pt+1.43- is bonded in a 6-coordinate geometry to three Pr3+, two equivalent Pt+1.43-, and three equivalent Sb+0.25+ atoms. There are two shorter (2.70 Å) and one longer (2.79 Å) Pt–Sb bond lengths. In the fourth Pt+1.43- site, Pt+1.43- is bonded in a 12-coordinate geometry to four equivalent Pr3+, four equivalent Pt+1.43-, and two equivalent Sb+0.25+ atoms. Both Pt–Sb bond lengths are 2.77 Å. There are two inequivalent Sb+0.25+ sites. In the first Sb+0.25+ site, Sb+0.25+ is bonded in a 6-coordinate geometry to six Pt+1.43- atoms. In the second Sb+0.25+ site, Sb+0.25+ is bonded to five Pt+1.43- atoms to form a mixture of distorted corner and edge-sharing SbPt5 trigonal bipyramids.
DOI: 10.15131/shef.data.12854975
title: Femoral neck strain prediction during level walking using a combined musculoskeletal and finite element model approach

description: The full of set of data contains; peak first and third principal strains at the femoral neck as predicted by the FE model, hip and knee joint contact forces personolised by the body weight, and Gluteus Medius muscle forces as calculated by the musculoskeletal model. Those are reported for the five cases and along the 100% of one gait cycle.<br>The study was approved by the Health Research Authority of East of England (Cambridgeshire and Hertfordshire Research Ethics Committee, reference 16/EE/0049).
DOI: 10.17188/1708585
title: Materials Data on TmAgTe2 by Materials Project

description: TmAgTe2 crystallizes in the tetragonal P-42_1m space group. The structure is three-dimensional. Tm3+ is bonded to six equivalent Te2- atoms to form TmTe6 octahedra that share corners with eight equivalent TmTe6 octahedra, corners with four equivalent AgTe4 tetrahedra, edges with two equivalent TmTe6 octahedra, and edges with four equivalent AgTe4 tetrahedra. The corner-sharing octahedra tilt angles range from 42–56°. There are a spread of Tm–Te bond distances ranging from 3.02–3.13 Å. Ag1+ is bonded to four equivalent Te2- atoms to form distorted AgTe4 tetrahedra that share corners with four equivalent TmTe6 octahedra, corners with four equivalent AgTe4 tetrahedra, and edges with four equivalent TmTe6 octahedra. The corner-sharing octahedral tilt angles are 62°. All Ag–Te bond lengths are 2.89 Å. Te2- is bonded in a 5-coordinate geometry to three equivalent Tm3+ and two equivalent Ag1+ atoms.
DOI: 10.15131/shef.data.12854975.v1
title: Femoral neck strain prediction during level walking using a combined musculoskeletal and finite element model approach

description: The full of set of data contains; peak first and third principal strains at the femoral neck as predicted by the FE model, hip and knee joint contact forces personolised by the body weight, and Gluteus Medius muscle forces as calculated by the musculoskeletal model. Those are reported for the five cases and along the 100% of one gait cycle.<br>The study was approved by the Health Research Authority of East of England (Cambridgeshire and Hertfordshire Research Ethics Committee, reference 16/EE/0049).