Engineering Papers⌕ Search

SEARCH · Engineering Papers

Results for “F-Fe-Li”

Search indexed NASA NTRS and DOE OSTI research on propulsion, heat transfer, battery materials and energy systems. Follow report and document links to the original sources.

Quote a phrase for an exact phrase match. Source license links do not imply unrestricted reuse.

159 records · Page 9

Materials Data on Li2Fe3F8 by Materials Project

Li2Fe3F8 crystallizes in the orthorhombic Cmce space group. The structure is three-dimensional. Li1+ is bonded to four F1- atoms to form LiF4 tetrahedra that share corners with nine FeF6 octahedra. The corner-sharing octahedra tilt angles range from 53–57°. There are a spread of Li–F bond distances ranging from 1.89–1.99 Å. There are two inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with six equivalent LiF4 tetrahedra and edges with four FeF6 octahedra. There are a spread of Fe–F bond distances ranging from 2.04–2.23 Å. In the second Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with six equivalent LiF4 tetrahedra and edges with four equivalent FeF6 octahedra. There are four shorter (2.10 Å) and two longer (2.12 Å) Fe–F bond lengths. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two Fe2+ atoms. In the second F1- site, F1- is bonded in a rectangular see-saw-like geometry to one Li1+ and three Fe2+ atoms. In the third F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two equivalent Fe2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiFeF3 by Materials Project

LiFeF3 is Ilmenite-like structured and crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.98–2.31 Å. In the second Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.97–2.30 Å. In the third Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.95–2.30 Å. In the fourth Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.96–2.28 Å. There are four inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to six F1- atoms to form distorted corner-sharing FeF6 octahedra. The corner-sharing octahedra tilt angles range from 49–52°. There are a spread of Fe–F bond distances ranging from 2.08–2.13 Å. In the second Fe2+ site, Fe2+ is bonded to six F1- atoms to form distorted corner-sharing FeF6 octahedra. The corner-sharing octahedra tilt angles range from 48–54°. There are a spread of Fe–F bond distances ranging from 2.09–2.14 Å. In the third Fe2+ site, Fe2+ is bonded to six F1- atoms to form corner-sharing FeF6 octahedra. The corner-sharing octahedra tilt angles range from 49–54°. There are a spread of Fe–F bond distances ranging from 2.09–2.13 Å. In the fourth Fe2+ site, Fe2+ is bonded to six F1- atoms to form distorted corner-sharing FeF6 octahedra. The corner-sharing octahedra tilt angles range from 48–54°. There are a spread of Fe–F bond distances ranging from 2.07–2.13 Å. There are twelve inequivalent F1- sites. In the first F1- site, F1- is bonded to two Li1+ and two Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLi2Fe2 trigonal pyramids. In the second F1- site, F1- is bonded to two Li1+ and two Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLi2Fe2 trigonal pyramids. In the third F1- site, F1- is bonded to two Li1+ and two Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLi2Fe2 trigonal pyramids. In the fourth F1- site, F1- is bonded to two Li1+ and two Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLi2Fe2 trigonal pyramids. In the fifth F1- site, F1- is bonded to two Li1+ and two Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLi2Fe2 trigonal pyramids. In the sixth F1- site, F1- is bonded to two Li1+ and two Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLi2Fe2 trigonal pyramids. In the seventh F1- site, F1- is bonded to two Li1+ and two Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLi2Fe2 trigonal pyramids. In the eighth F1- site, F1- is bonded to two Li1+ and two Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLi2Fe2 trigonal pyramids. In the ninth F1- site, F1- is bonded to two Li1+ and two Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLi2Fe2 trigonal pyramids. In the tenth F1- site, F1- is bonded to two Li1+ and two Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLi2Fe2 trigonal pyramids. In the eleventh F1- site, F1- is bonded to two Li1+ and two Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLi2Fe2 trigonal pyramids. In the twelfth F1- site, F1- is bonded to two Li1+ and two Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLi2Fe2 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on LiFeF3 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on Li3Fe4F19 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on Li2FeF4 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on Li2FeF4 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on LiFe2F5 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on LiFeF5 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on Li2FeF5 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on LiFeF3 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on Li2Fe3F8 by Materials Project

Li2Fe3F8 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 3-coordinate geometry to five F1- atoms. There are a spread of Li–F bond distances ranging from 1.86–2.66 Å. In the second Li1+ site, Li1+ is bonded to four F1- atoms to form distorted LiF4 trigonal pyramids that share corners with seven FeF6 octahedra. The corner-sharing octahedra tilt angles range from 51–76°. There are a spread of Li–F bond distances ranging from 1.89–2.31 Å. In the third Li1+ site, Li1+ is bonded to four F1- atoms to form distorted LiF4 trigonal pyramids that share corners with seven FeF6 octahedra. The corner-sharing octahedra tilt angles range from 50–77°. There are a spread of Li–F bond distances ranging from 1.89–2.31 Å. In the fourth Li1+ site, Li1+ is bonded in a 3-coordinate geometry to five F1- atoms. There are a spread of Li–F bond distances ranging from 1.86–2.68 Å. There are six inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with two LiF4 trigonal pyramids and edges with six FeF6 octahedra. There are a spread of Fe–F bond distances ranging from 2.03–2.18 Å. In the second Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share a cornercorner with one LiF4 trigonal pyramid and edges with six FeF6 octahedra. There are a spread of Fe–F bond distances ranging from 2.04–2.16 Å. In the third Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share a cornercorner with one LiF4 trigonal pyramid and edges with six FeF6 octahedra. There are a spread of Fe–F bond distances ranging from 2.04–2.16 Å. In the fourth Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with two LiF4 trigonal pyramids and edges with six FeF6 octahedra. There are a spread of Fe–F bond distances ranging from 2.03–2.18 Å. In the fifth Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with four LiF4 trigonal pyramids and edges with two equivalent FeF6 octahedra. There are a spread of Fe–F bond distances ranging from 2.06–2.18 Å. In the sixth Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with four LiF4 trigonal pyramids and edges with two equivalent FeF6 octahedra. There are a spread of Fe–F bond distances ranging from 2.06–2.18 Å. There are sixteen inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal non-coplanar geometry to one Li1+ and two Fe2+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two Fe2+ atoms. In the third F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one Fe2+ atom. In the fourth F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one Fe2+ atom. In the fifth F1- site, F1- is bonded to one Li1+ and three Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLiFe3 trigonal pyramids. In the sixth F1- site, F1- is bonded in a distorted trigonal non-coplanar geometry to three Fe2+ atoms. In the seventh F1- site, F1- is bonded to one Li1+ and three Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLiFe3 trigonal pyramids. In the eighth F1- site, F1- is bonded to one Li1+ and three Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLiFe3 trigonal pyramids. In the ninth F1- site, F1- is bonded to one Li1+ and three Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLiFe3 trigonal pyramids. In the tenth F1- site, F1- is bonded to one Li1+ and three Fe2+ atoms to form a mixture of distorted edge and corner-sharing FLiFe3 trigonal pyramids. In the eleventh F1- site, F1- is bonded in a distorted trigonal non-coplanar geometry to three Fe2+ atoms. In the twelfth F1- site, F1- is bonded in a 4-coordinate geometry to one Li1+ and three Fe2+ atoms. In the thirteenth F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one Fe2+ atom. In the fourteenth F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one Fe2+ atom. In the fifteenth F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two Fe2+ atoms. In the sixteenth F1- site, F1- is bonded in a distorted trigonal non-coplanar geometry to one Li1+ and two Fe2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiFeF3 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on LiFeF5 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on LiFeF3 by Materials Project

LiFeF3 is pyrite-derived structured and crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Li1+ is bonded to five F1- atoms to form distorted LiF5 tetrahedra that share corners with six FeF6 octahedra, corners with four equivalent LiF5 tetrahedra, and edges with two FeF6 octahedra. The corner-sharing octahedra tilt angles range from 53–71°. There are a spread of Li–F bond distances ranging from 1.93–2.53 Å. There are two inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with two equivalent FeF6 octahedra, corners with six equivalent LiF5 tetrahedra, edges with two equivalent FeF6 octahedra, and edges with two equivalent LiF5 tetrahedra. The corner-sharing octahedral tilt angles are 64°. There are a spread of Fe–F bond distances ranging from 2.08–2.17 Å. In the second Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with two equivalent FeF6 octahedra, corners with six equivalent LiF5 tetrahedra, edges with two equivalent FeF6 octahedra, and edges with two equivalent LiF5 tetrahedra. The corner-sharing octahedral tilt angles are 64°. There are a spread of Fe–F bond distances ranging from 2.05–2.17 Å. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a 3-coordinate geometry to one Li1+ and two Fe2+ atoms. In the second F1- site, F1- is bonded to two equivalent Li1+ and two Fe2+ atoms to form corner-sharing FLi2Fe2 tetrahedra. In the third F1- site, F1- is bonded in a 4-coordinate geometry to two equivalent Li1+ and two Fe2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiFeF3 by Materials Project

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

36 MATERIALS SCIENCE↗