Engineering Papers⌕ Search

SEARCH · Engineering Papers

Results for “F-Fe-Li-O”

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.

At least 73 records · Page 4

Materials Data on Li11Fe5(OF11)2 by Materials Project

Li11Fe5(OF11)2 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are eleven inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four F1- atoms to form LiF4 tetrahedra that share corners with three LiOF5 octahedra, corners with four FeOF5 octahedra, and corners with two equivalent LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 49–71°. There are a spread of Li–F bond distances ranging from 1.89–1.93 Å. In the second Li1+ site, Li1+ is bonded to one O2- and five F1- atoms to form LiOF5 octahedra that share corners with three LiF4 tetrahedra, edges with three LiF6 octahedra, and edges with three FeF6 octahedra. The Li–O bond length is 2.05 Å. There are a spread of Li–F bond distances ranging from 1.95–2.21 Å. In the third Li1+ site, Li1+ is bonded to six F1- atoms to form distorted LiF6 octahedra that share corners with two LiF6 octahedra, corners with four FeOF5 octahedra, a cornercorner with one LiF4 tetrahedra, an edgeedge with one FeF6 octahedra, and edges with two LiOF5 octahedra. The corner-sharing octahedra tilt angles range from 7–56°. There are a spread of Li–F bond distances ranging from 1.95–2.47 Å. In the fourth Li1+ site, Li1+ is bonded to six F1- atoms to form LiF6 octahedra that share corners with two LiF6 octahedra, corners with three LiF4 tetrahedra, edges with three LiOF5 octahedra, and edges with three FeF6 octahedra. The corner-sharing octahedra tilt angles range from 8–57°. There are a spread of Li–F bond distances ranging from 1.95–2.16 Å. In the fifth Li1+ site, Li1+ is bonded to four F1- atoms to form LiF4 tetrahedra that share corners with four LiOF5 octahedra, corners with four FeOF5 octahedra, and corners with two equivalent LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 48–66°. There are a spread of Li–F bond distances ranging from 1.89–1.93 Å. In the sixth Li1+ site, Li1+ is bonded to four F1- atoms to form LiF4 tetrahedra that share corners with four LiF6 octahedra, corners with four FeF6 octahedra, and corners with two equivalent LiOF3 tetrahedra. The corner-sharing octahedra tilt angles range from 54–67°. There are a spread of Li–F bond distances ranging from 1.89–1.92 Å. In the seventh Li1+ site, Li1+ is bonded to six F1- atoms to form LiF6 octahedra that share corners with two LiF6 octahedra, corners with three LiF4 tetrahedra, edges with three LiOF5 octahedra, and edges with three FeOF5 octahedra. The corner-sharing octahedra tilt angles range from 17–56°. There are a spread of Li–F bond distances ranging from 2.00–2.09 Å. In the eighth Li1+ site, Li1+ is bonded to six F1- atoms to form distorted LiF6 octahedra that share corners with two LiF6 octahedra, corners with four FeOF5 octahedra, a cornercorner with one LiF4 tetrahedra, an edgeedge with one FeF6 octahedra, and edges with two LiOF5 octahedra. The corner-sharing octahedra tilt angles range from 9–57°. There are a spread of Li–F bond distances ranging from 1.98–2.44 Å. In the ninth Li1+ site, Li1+ is bonded in a 6-coordinate geometry to five F1- atoms. There are a spread of Li–F bond distances ranging from 1.96–2.12 Å. In the tenth Li1+ site, Li1+ is bonded to one O2- and five F1- atoms to form LiOF5 octahedra that share corners with three LiF4 tetrahedra, edges with three LiF6 octahedra, and edges with three FeOF5 octahedra. The Li–O bond length is 2.01 Å. There are a spread of Li–F bond distances ranging from 2.02–2.12 Å. In the eleventh Li1+ site, Li1+ is bonded to one O2- and three F1- atoms to form LiOF3 tetrahedra that share corners with three LiOF5 octahedra, corners with four FeOF5 octahedra, and corners with two equivalent LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 52–71°. The Li–O bond length is 1.95 Å. There are a spread of Li–F bond distances ranging from 1.88–1.94 Å. There are five inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded to one O2- and five F1- atoms to form FeOF5 octahedra that share corners with two LiF6 octahedra, corners with four LiF4 tetrahedra, and edges with three LiOF5 octahedra. The corner-sharing octahedra tilt angles range from 9–52°. The Fe–O bond length is 1.87 Å. There are a spread of Fe–F bond distances ranging from 1.95–2.07 Å. In the second Fe3+ site, Fe3+ is bonded in a 6-coordinate geometry to two O2- and four F1- atoms. There is one shorter (1.84 Å) and one longer (1.90 Å) Fe–O bond length. There are a spread of Fe–F bond distances ranging from 2.03–2.53 Å. In the third Fe3+ site, Fe3+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with two equivalent LiF6 octahedra, corners with four LiF4 tetrahedra, and edges with four LiOF5 octahedra. The corner-sharing octahedra tilt angles range from 48–56°. There are a spread of Fe–F bond distances ranging from 1.92–2.00 Å. In the fourth Fe3+ site, Fe3+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with two equivalent LiF6 octahedra, corners with four LiF4 tetrahedra, and edges with four LiOF5 octahedra. The corner-sharing octahedra tilt angles range from 48–51°. There are a spread of Fe–F bond distances ranging from 1.91–2.09 Å. In the fifth Fe3+ site, Fe3+ is bonded to one O2- and five F1- atoms to form distorted FeOF5 octahedra that share corners with two LiF6 octahedra, corners with four LiF4 tetrahedra, and edges with three LiOF5 octahedra. The corner-sharing octahedra tilt angles range from 7–51°. The Fe–O bond length is 1.91 Å. There are a spread of Fe–F bond distances ranging from 1.92–2.29 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+ and two Fe3+ atoms. In the second O2- site, O2- is bonded to two Li1+ and two Fe3+ atoms to form OLi2Fe2 tetrahedra that share a cornercorner with one FLi3Fe2 square pyramid, corners with two FLi3Fe tetrahedra, edges with two FLi3Fe2 square pyramids, and an edgeedge with one FLi3Fe tetrahedra. There are twenty-two inequivalent F1- sites. In the first F1- site, F1- is bonded in a trigonal planar geometry to one Li1+ and two Fe3+ atoms. In the second F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one Fe3+ atom. In the third F1- site, F1- is bonded to three Li1+ and two Fe3+ atoms to form distorted FLi3Fe2 square pyramids that share a cornercorner with one OLi2Fe2 tetrahedra, a cornercorner with one FLi3Fe tetrahedra, edges with two equivalent FLi3Fe2 square pyramids, an edgeedge with one OLi2Fe2 tetrahedra, and edges with three FLi3Fe tetrahedra. In the fourth F1- site, F1- is bonded to three Li1+ and one Fe3+ atom to form distorted FLi3Fe tetrahedra that share a cornercorner with one FLi3Fe2 square pyramid, corners with four FLi3Fe tetrahedra, edges with two FLi3Fe2 square pyramids, and an edgeedge with one OLi2Fe2 tetrahedra. In the fifth F1- site, F1- is bonded to three Li1+ and one Fe3+ atom to form FLi3Fe tetrahedra that share a cornercorner with one FLi3Fe2 square pyramid, a cornercorner with one OLi2Fe2 tetrahedra, corners with three FLi3Fe tetrahedra, edges with two FLi3Fe2 square pyramids, and an edgeedge with one FLi3Fe tetrahedra. In the sixth F1- site, F1- is bonded to three Li1+ and two Fe3+ atoms to form distorted FLi3Fe2 square pyramids that share corners with two FLi3Fe tetrahedra, edges with two equivalent FLi3Fe2 square pyramids, an edgeedge with one OLi2Fe2 tetrahedra, and edges with three FLi3Fe tetrahedra. In the seventh F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one Fe3+ atom. In the eighth F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two Fe3+ atoms. In the ninth F1- site, F1- is bonded to three Li1+ and one Fe3+ atom to form FLi3Fe tetrahedra that share a cornercorner with one FLi3Fe2 square pyramid, a cornercorner with one FLi3Fe tetrahedra, a cornercorner with one FLi3Fe trigonal pyramid, edges with two FLi3Fe2 square pyramids, and an edgeedge with one FLi3Fe tetrahedra. In the tenth F1- site, F1- is bonded in a distorted trigonal planar geometry to two Li1+ and one Fe3+ atom. In the eleventh F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one Fe3+ atom. In the twelfth F1- site, F1- is bonded to three Li1+ and one Fe3+ atom to form distorted FLi3Fe tetrahedra that share corners with two FLi3Fe tetrahedra, an edgeedge with one FLi4Fe square pyramid, and an edgeedge with one FLi3Fe trigonal pyramid. In the thirteenth F1- site, F1- is bonded in a distorted trigonal planar geometry to two Li1+ and one Fe3+ atom. In the fourteenth F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one Fe3+ atom. In the fifteenth F1- site, F1- is bonded in a 5-coordinate geometry to three Li1+ and one Fe3+ atom. In the sixteenth F1- site, F1- is bonded to three Li1+ and one Fe3+ atom to form distorted FLi3Fe trigonal pyramids that share corners with four FLi3Fe tetrahedra, an edgeedge with one FLi4Fe square pyramid, and an edgeedge with one FLi3Fe tetrahedra. In the seventeenth F1- site, F1- is bonded to three Li1+ and one Fe3+ atom to form distorted FLi3Fe tetrahedra that share a cornercorner with one FLi4Fe square pyramid, a cornercorner with one OLi2Fe2 tetrahedra, a cornercorner with one FLi3Fe tetrahedra, corners with two equivalent FLi3Fe trigonal pyramids, an edgeedge with one FLi4Fe square pyramid, and an edgeedge with one FLi3Fe tetrahedra. In the eighteenth F1- site, F1- is bonded to four Li1+ and one Fe3+ atom to form a mixture of distorted edge and corner-sharing FLi4Fe square pyramids. In the nineteenth F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one Fe3+ atom. In the twentieth F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one Fe3+ atom. In the twenty-first F1- site, F1- is bonded to three Li1+ and one Fe3+ atom to form FLi3Fe tetrahedra that share a cornercorner with one FLi4Fe square pyramid, a cornercorner with one FLi3Fe tetrahedra, a cornercorner with one FLi3Fe trigonal pyramid, an edgeedge with one FLi4Fe square pyramid, and an edgeedge with one FLi3Fe tetrahedra. In the twenty-second F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one Fe3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li7FeO5F 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 LiFe2OF3 by Materials Project

LiFe2OF3 is Ilmenite-derived structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Li1+ is bonded to one O2- and three F1- atoms to form distorted LiOF3 tetrahedra that share corners with six FeO2F4 octahedra and edges with three FeO2F4 octahedra. The corner-sharing octahedra tilt angles range from 60–65°. The Li–O bond length is 1.86 Å. There is one shorter (1.97 Å) and two longer (2.00 Å) Li–F bond length. There are three inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to two equivalent O2- and four F1- atoms to form FeO2F4 octahedra that share corners with four equivalent FeF6 octahedra, corners with two equivalent LiOF3 tetrahedra, edges with four FeO2F4 octahedra, and edges with two equivalent LiOF3 tetrahedra. The corner-sharing octahedra tilt angles range from 50–52°. Both Fe–O bond lengths are 1.96 Å. There are two shorter (2.30 Å) and two longer (2.36 Å) Fe–F bond lengths. In the second Fe2+ site, Fe2+ is bonded to two equivalent O2- and four equivalent F1- atoms to form FeO2F4 octahedra that share corners with four equivalent FeF6 octahedra, corners with two equivalent LiOF3 tetrahedra, edges with four equivalent FeO2F4 octahedra, and edges with two equivalent LiOF3 tetrahedra. The corner-sharing octahedral tilt angles are 48°. Both Fe–O bond lengths are 2.04 Å. All Fe–F bond lengths are 2.23 Å. In the third Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with twelve FeO2F4 octahedra and corners with six equivalent LiOF3 tetrahedra. The corner-sharing octahedra tilt angles range from 48–52°. There are four shorter (2.15 Å) and two longer (2.16 Å) Fe–F bond lengths. O2- is bonded to one Li1+ and three Fe2+ atoms to form corner-sharing OLiFe3 tetrahedra. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted rectangular see-saw-like geometry to one Li1+ and three Fe2+ atoms. In the second F1- site, F1- is bonded in a rectangular see-saw-like geometry to one Li1+ and three Fe2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Li4FeO3F 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 LiFe2OF3 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 Li2FeOF3 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 LiFeOF2 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 Li3Fe(OF)2 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 LiFe2OF3 by Materials Project

LiFe2OF3 is Spinel-derived structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Li1+ is bonded to one O2- and three equivalent F1- atoms to form LiOF3 tetrahedra that share corners with twelve FeF6 octahedra. The corner-sharing octahedra tilt angles range from 53–63°. The Li–O bond length is 1.99 Å. All Li–F bond lengths are 1.98 Å. There are two inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to two equivalent O2- and four equivalent F1- atoms to form FeO2F4 octahedra that share corners with six equivalent LiOF3 tetrahedra and edges with six FeF6 octahedra. Both Fe–O bond lengths are 2.00 Å. All Fe–F bond lengths are 2.27 Å. In the second Fe2+ site, Fe2+ is bonded to six equivalent F1- atoms to form FeF6 octahedra that share corners with six equivalent LiOF3 tetrahedra and edges with six equivalent FeO2F4 octahedra. All Fe–F bond lengths are 2.12 Å. O2- is bonded to one Li1+ and three equivalent Fe2+ atoms to form corner-sharing OLiFe3 tetrahedra. F1- is bonded in a rectangular see-saw-like geometry to one Li1+ and three Fe2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiFe2OF3 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 Li3FeOF3 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 Li3Fe9O5F11 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 LiFeOF 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 LiFe2O2F3 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 Li5FeO3F2 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 Li3Fe4(OF3)3 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 Li3FeOF3 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 LiFe2O2F3 by Materials Project

LiFe2O2F3 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. Li1+ is bonded to two equivalent O2- and four F1- atoms to form LiO2F4 octahedra that share corners with two equivalent LiO2F4 octahedra, corners with six equivalent FeO3F3 octahedra, and edges with four equivalent FeO3F3 octahedra. The corner-sharing octahedra tilt angles range from 43–62°. Both Li–O bond lengths are 2.15 Å. There are two shorter (2.03 Å) and two longer (2.06 Å) Li–F bond lengths. Fe3+ is bonded to three equivalent O2- and three F1- atoms to form FeO3F3 octahedra that share corners with three equivalent LiO2F4 octahedra, corners with four equivalent FeO3F3 octahedra, an edgeedge with one FeO3F3 octahedra, edges with two equivalent LiO2F4 octahedra, and a faceface with one FeO3F3 octahedra. The corner-sharing octahedra tilt angles range from 43–48°. There are a spread of Fe–O bond distances ranging from 1.92–1.94 Å. There are a spread of Fe–F bond distances ranging from 1.95–2.05 Å. O2- is bonded to one Li1+ and three equivalent Fe3+ atoms to form a mixture of edge and corner-sharing OLiFe3 trigonal pyramids. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted T-shaped geometry to one Li1+ and two equivalent Fe3+ atoms. In the second F1- site, F1- is bonded in a 4-coordinate geometry to two equivalent Li1+ and two equivalent Fe3+ atoms.

36 MATERIALS SCIENCE↗