Engineering Papers⌕ Search

SEARCH · Engineering Papers

Results for “F-Li-O-V”

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 109 records · Page 6

Materials Data on LiV3O3F7 by Materials Project

LiV3O3F7 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four F1- atoms. There are a spread of Li–F bond distances ranging from 1.88–2.13 Å. In the second Li1+ site, Li1+ is bonded in a 4-coordinate geometry to one O2- and three F1- atoms. The Li–O bond length is 2.25 Å. There are a spread of Li–F bond distances ranging from 1.90–2.08 Å. There are six inequivalent V4+ sites. In the first V4+ site, V4+ is bonded to three O2- and three F1- atoms to form distorted corner-sharing VO3F3 octahedra. The corner-sharing octahedra tilt angles range from 16–42°. There are a spread of V–O bond distances ranging from 1.68–2.15 Å. There are a spread of V–F bond distances ranging from 1.88–2.02 Å. In the second V4+ site, V4+ is bonded to two O2- and four F1- atoms to form corner-sharing VO2F4 octahedra. The corner-sharing octahedra tilt angles range from 7–38°. There is one shorter (1.98 Å) and one longer (2.01 Å) V–O bond length. There are a spread of V–F bond distances ranging from 1.88–2.02 Å. In the third V4+ site, V4+ is bonded to one O2- and five F1- atoms to form corner-sharing VOF5 octahedra. The corner-sharing octahedra tilt angles range from 7–48°. The V–O bond length is 1.67 Å. There are a spread of V–F bond distances ranging from 1.93–2.08 Å. In the fourth V4+ site, V4+ is bonded to two O2- and four F1- atoms to form corner-sharing VO2F4 octahedra. The corner-sharing octahedra tilt angles range from 15–41°. There is one shorter (1.68 Å) and one longer (1.73 Å) V–O bond length. There are a spread of V–F bond distances ranging from 1.85–2.05 Å. In the fifth V4+ site, V4+ is bonded to two O2- and four F1- atoms to form distorted corner-sharing VO2F4 octahedra. The corner-sharing octahedra tilt angles range from 13–48°. There is one shorter (1.68 Å) and one longer (2.13 Å) V–O bond length. There are a spread of V–F bond distances ranging from 1.88–2.02 Å. In the sixth V4+ site, V4+ is bonded to two O2- and four F1- atoms to form distorted corner-sharing VO2F4 octahedra. The corner-sharing octahedra tilt angles range from 13–41°. There is one shorter (1.69 Å) and one longer (1.99 Å) V–O bond length. There are three shorter (1.94 Å) and one longer (2.14 Å) V–F bond lengths. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to two V4+ atoms. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the third O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two V4+ atoms. In the fourth O2- site, O2- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the fifth O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+ and two V4+ atoms. In the sixth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two V4+ atoms. There are fourteen inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted linear geometry to two V4+ atoms. In the second F1- site, F1- is bonded in a bent 150 degrees geometry to one Li1+ and one V4+ atom. In the third F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two V4+ atoms. In the fourth F1- site, F1- is bonded in a distorted linear geometry to two V4+ atoms. In the fifth F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the sixth F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two V4+ atoms. In the seventh F1- site, F1- is bonded in a linear geometry to one Li1+ and one V4+ atom. In the eighth F1- site, F1- is bonded in a linear geometry to two V4+ atoms. In the ninth F1- site, F1- is bonded in a distorted linear geometry to two V4+ atoms. In the tenth F1- site, F1- is bonded in a bent 150 degrees geometry to one Li1+ and one V4+ atom. In the eleventh F1- site, F1- is bonded in a distorted bent 150 degrees geometry to two V4+ atoms. In the twelfth F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two V4+ atoms. In the thirteenth F1- site, F1- is bonded in a bent 150 degrees geometry to one Li1+ and one V4+ atom. In the fourteenth F1- site, F1- is bonded in a distorted linear geometry to two V4+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiV3OF11 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 LiV2OF5 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 LiV2OF7 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 LiVOF3 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 LiV2OF7 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 LiV2OF5 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 Li4V3(OF2)4 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 LiV2OF5 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 LiV3OF11 by Materials Project

LiV3OF11 crystallizes in the triclinic P1 space group. The structure is two-dimensional and consists of one LiV3OF11 sheet oriented in the (0, 0, 1) direction. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 5-coordinate geometry to one O2- and four F1- atoms. The Li–O bond length is 2.14 Å. There are a spread of Li–F bond distances ranging from 1.81–2.63 Å. In the second Li1+ site, Li1+ is bonded in a 4-coordinate geometry to one O2- and three F1- atoms. The Li–O bond length is 1.91 Å. There are a spread of Li–F bond distances ranging from 1.89–2.13 Å. There are six inequivalent V4+ sites. In the first V4+ site, V4+ is bonded to one O2- and five F1- atoms to form corner-sharing VOF5 octahedra. The corner-sharing octahedra tilt angles range from 29–31°. The V–O bond length is 1.66 Å. There are a spread of V–F bond distances ranging from 1.85–2.04 Å. In the second V4+ site, V4+ is bonded to one O2- and five F1- atoms to form corner-sharing VOF5 octahedra. The corner-sharing octahedra tilt angles range from 23–30°. The V–O bond length is 2.05 Å. There are a spread of V–F bond distances ranging from 1.75–1.98 Å. In the third V4+ site, V4+ is bonded to six F1- atoms to form corner-sharing VF6 octahedra. The corner-sharing octahedra tilt angles range from 29–34°. There are a spread of V–F bond distances ranging from 1.87–2.07 Å. In the fourth V4+ site, V4+ is bonded to six F1- atoms to form corner-sharing VF6 octahedra. The corner-sharing octahedra tilt angles range from 29–31°. There are a spread of V–F bond distances ranging from 1.76–1.95 Å. In the fifth V4+ site, V4+ is bonded to one O2- and five F1- atoms to form distorted corner-sharing VOF5 octahedra. The corner-sharing octahedra tilt angles range from 23–30°. The V–O bond length is 1.71 Å. There are a spread of V–F bond distances ranging from 1.75–2.20 Å. In the sixth V4+ site, V4+ is bonded to six F1- atoms to form corner-sharing VF6 octahedra. The corner-sharing octahedra tilt angles range from 29–34°. There are a spread of V–F bond distances ranging from 1.77–1.96 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Li1+ and one V4+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+ and two V4+ atoms. There are twenty-two inequivalent F1- sites. In the first F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the second F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the third F1- site, F1- is bonded in a distorted bent 150 degrees geometry to two V4+ atoms. In the fourth F1- site, F1- is bonded in a bent 120 degrees geometry to one Li1+ and one V4+ atom. In the fifth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the sixth F1- site, F1- is bonded in a water-like geometry to one Li1+ and one V4+ atom. In the seventh F1- site, F1- is bonded in a water-like geometry to one Li1+ and one V4+ atom. In the eighth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the ninth F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the tenth F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the eleventh F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the twelfth F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the thirteenth F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the fourteenth F1- site, F1- is bonded in a bent 120 degrees geometry to one Li1+ and one V4+ atom. In the fifteenth F1- site, F1- is bonded in a bent 120 degrees geometry to one Li1+ and one V4+ atom. In the sixteenth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the seventeenth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the eighteenth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the nineteenth F1- site, F1- is bonded in a distorted single-bond geometry to one Li1+ and one V4+ atom. In the twentieth F1- site, F1- is bonded in a distorted T-shaped geometry to one Li1+ and two V4+ atoms. In the twenty-first F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the twenty-second F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Li2VOF4 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 Li7VO5F 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 Li6V(OF)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 Li11V6O5F19 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 Li2V3(OF)4 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 LiV3OF11 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 Li2VO2F 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 Li2V(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↗