Search NASA⌕ Search

DOE OSTI · 1305653

Materials Data on VO2F by Materials Project

Abstract

FVO2 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent V5+ sites. In the first V5+ site, V5+ is bonded in a 6-coordinate geometry to four O2- and two F1- atoms. There are a spread of V–O bond distances ranging from 1.64–2.27 Å. There is one shorter (1.94 Å) and one longer (1.96 Å) V–F bond length. In the second V5+ site, V5+ is bonded in a 6-coordinate geometry to four O2- and two F1- atoms. There are a spread of V–O bond distances ranging from 1.66–2.30 Å. There are one shorter (2.04 Å) and one longer (2.07 Å) V–F bond lengths. In the third V5+ site, V5+ is bonded to four O2- and two F1- atoms to form distorted corner-sharing VO4F2 octahedra. The corner-sharing octahedra tilt angles range from 7–37°. There are a spread of V–O bond distances ranging from 1.65–2.21 Å. There are one shorter (1.95 Å) and one longer (2.13 Å) V–F bond lengths. In the fourth V5+ site, V5+ is bonded to four O2- and two F1- atoms to form distorted corner-sharing VO4F2 octahedra. The corner-sharing octahedra tilt angles range from 7–37°. There are a spread of V–O bond distances ranging from 1.64–2.26 Å. There is one shorter (1.89 Å) and one longer (1.98 Å) V–F bond length. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two V5+ atoms. In the second O2- site, O2- is bonded in a distorted single-bond geometry to two V5+ atoms. In the third O2- site, O2- is bonded in a distorted single-bond geometry to two V5+ atoms. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to two V5+ atoms. In the fifth O2- site, O2- is bonded in a distorted single-bond geometry to two V5+ atoms. In the sixth O2- site, O2- is bonded in a linear geometry to two V5+ atoms. In the seventh O2- site, O2- is bonded in a bent 150 degrees geometry to two V5+ atoms. In the eighth O2- site, O2- is bonded in a linear geometry to two V5+ atoms. There are four inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted bent 150 degrees geometry to two V5+ atoms. In the second F1- site, F1- is bonded in a linear geometry to two V5+ atoms. In the third F1- site, F1- is bonded in a distorted bent 150 degrees geometry to two V5+ atoms. In the fourth F1- site, F1- is bonded in a distorted bent 150 degrees geometry to two V5+ atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-07-22. Materials Data on VO2F by Materials Project. https://doi.org/10.17188/1305653

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↗