Search NASA⌕ Search

DOE OSTI · 1307559

Materials Data on LiV8F33 by Materials Project

Abstract

LiV8F33 crystallizes in the monoclinic Cc space group. The structure is two-dimensional and consists of two LiV8F33 sheets oriented in the (0, 0, 1) direction. Li1+ is bonded in a distorted T-shaped geometry to three F1- atoms. There is two shorter (1.90 Å) and one longer (1.91 Å) Li–F bond length. There are eight inequivalent V4+ sites. In the first V4+ site, V4+ is bonded to six F1- atoms to form corner-sharing VF6 octahedra. The corner-sharing octahedra tilt angles range from 28–31°. There are a spread of V–F bond distances ranging from 1.74–2.00 Å. In the second V4+ site, V4+ is bonded to six F1- atoms to form corner-sharing VF6 octahedra. The corner-sharing octahedra tilt angles range from 29–33°. There are a spread of V–F bond distances ranging from 1.75–2.03 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 28–33°. There are a spread of V–F bond distances ranging from 1.75–2.03 Å. In the fourth V4+ site, V4+ is bonded to six F1- atoms to form corner-sharing VF6 octahedra. The corner-sharing octahedral tilt angles are 33°. There are a spread of V–F bond distances ranging from 1.77–2.07 Å. In the fifth V4+ site, V4+ is bonded to six F1- atoms to form corner-sharing VF6 octahedra. The corner-sharing octahedra tilt angles range from 31–32°. There are a spread of V–F bond distances ranging from 1.77–2.06 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 28–32°. There are a spread of V–F bond distances ranging from 1.74–2.00 Å. In the seventh 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 1.74–2.00 Å. In the eighth V4+ site, V4+ is bonded to six F1- atoms to form corner-sharing VF6 octahedra. The corner-sharing octahedra tilt angles range from 28–33°. There are a spread of V–F bond distances ranging from 1.75–2.03 Å. There are thirty-three inequivalent F1- sites. In the first F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the second F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the third F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the fourth F1- site, F1- is bonded in a bent 150 degrees 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 bent 150 degrees geometry to two V4+ atoms. In the seventh F1- site, F1- is bonded in a bent 150 degrees geometry to one Li1+ and one V4+ atom. In the eighth F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the ninth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the tenth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the eleventh F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the twelfth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. 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 single-bond geometry to one V4+ atom. In the fifteenth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the sixteenth F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the seventeenth F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the eighteenth F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the nineteenth F1- site, F1- is bonded in a bent 150 degrees geometry to one Li1+ and one V4+ atom. In the twentieth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the twenty-first F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the twenty-second F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the twenty-third F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the twenty-fourth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the twenty-fifth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the twenty-sixth F1- site, F1- is bonded in a bent 150 degrees geometry to one Li1+ and one V4+ atom. In the twenty-seventh F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the twenty-eighth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the twenty-ninth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the thirtieth F1- site, F1- is bonded in a single-bond geometry to one V4+ atom. In the thirty-first F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the thirty-second F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms. In the thirty-third F1- site, F1- is bonded in a bent 150 degrees geometry to two V4+ atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-05-29. Materials Data on LiV8F33 by Materials Project. https://doi.org/10.17188/1307559

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related reports

Cyclic moisture reactivation of calcium sorbents for long duration thermochemical energy storage

The transition to a flexible and reliable energy infrastructure, using electro-thermal energy generation technologies such as geothermal, concentrated solar power, and nuclear, usually demands simultaneous advancement of thermal energy storage (TES) to support on-demand electricity generation and industrial applications while mitigating the inherent intermittency of renewable energy sources and power outages from direct energy generation. Among TES technologies, thermochemical energy storage (TCES) based on calcium looping emerges as a compelling high-power energy storage candidate due to its high reaction enthalpy, compatibility with elevated operating temperatures, and abundance of low-cost materials. However, the long-term durability of calcium-based sorbents for TCES is hindered by surface sintering and particle aggregation, leading to performance degradation over repeated thermal cycles. This study explores a moisture hydration-based strategy to regenerate a degraded calcium sorbent and mitigate performance degradation for long duration TCES. The addition of moisture transforms calcium oxide into calcium hydroxide and produces intercalation water layers, associated with a regenerated surface area and reduced calcium oxide crystallite size. Both these effects are beneficial in restoring the sorbents' reactivity for carbonization. Additionally, an optimized hydration-assisted reactivation protocol balances the recovered energy storage capacity with heating penalty required for moisture removal from hydrated samples, resulting in an enhanced energy storage capacity up to 176% compared to benchmark sorbents that undergo cycling without reactivation after 60 cycles. In conclusion, these results highlight the potential of hydration-assisted reactivation to enhance the long-term performance of TCES, providing an effective pathway to advancing electro-thermal storage technologies.

36 MATERIALS SCIENCE↗