Search NASA⌕ Search

DOE OSTI · 1300166

Materials Data on Li2CrPO4F by Materials Project

Abstract

Li2CrPO4F crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 6-coordinate geometry to four O2- and two F1- atoms. There are a spread of Li–O bond distances ranging from 2.07–2.34 Å. There are one shorter (1.89 Å) and one longer (2.34 Å) Li–F bond lengths. In the second Li1+ site, Li1+ is bonded in a 5-coordinate geometry to four O2- and one F1- atom. There are a spread of Li–O bond distances ranging from 2.07–2.21 Å. The Li–F bond length is 1.92 Å. In the third Li1+ site, Li1+ is bonded to four O2- and two F1- atoms to form distorted LiO4F2 octahedra that share a cornercorner with one LiO4F2 octahedra, corners with two CrO4F2 octahedra, corners with four PO4 tetrahedra, edges with two CrO4F2 octahedra, and a faceface with one LiO4F2 octahedra. The corner-sharing octahedra tilt angles range from 23–75°. There are a spread of Li–O bond distances ranging from 2.04–2.31 Å. There are one shorter (2.17 Å) and one longer (2.49 Å) Li–F bond lengths. There are two inequivalent Cr2+ sites. In the first Cr2+ site, Cr2+ is bonded to four O2- and two equivalent F1- atoms to form CrO4F2 octahedra that share corners with two equivalent LiO4F2 octahedra, corners with four PO4 tetrahedra, edges with two equivalent LiO4F2 octahedra, and edges with two equivalent CrO4F2 octahedra. The corner-sharing octahedral tilt angles are 40°. There are two shorter (2.07 Å) and two longer (2.16 Å) Cr–O bond lengths. Both Cr–F bond lengths are 2.32 Å. In the second Cr2+ site, Cr2+ is bonded to four O2- and two equivalent F1- atoms to form CrO4F2 octahedra that share corners with two equivalent LiO4F2 octahedra, corners with four PO4 tetrahedra, edges with two equivalent LiO4F2 octahedra, and edges with two equivalent CrO4F2 octahedra. The corner-sharing octahedral tilt angles are 23°. There are two shorter (2.08 Å) and two longer (2.11 Å) Cr–O bond lengths. Both Cr–F bond lengths are 2.36 Å. There are two inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with four equivalent LiO4F2 octahedra and corners with four CrO4F2 octahedra. The corner-sharing octahedra tilt angles range from 52–66°. There are a spread of P–O bond distances ranging from 1.55–1.58 Å. In the second P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with four equivalent LiO4F2 octahedra and corners with four CrO4F2 octahedra. The corner-sharing octahedra tilt angles range from 52–59°. There are a spread of P–O bond distances ranging from 1.53–1.58 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+, two equivalent Cr2+, and one P5+ atom. In the second O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two Li1+, one Cr2+, and one P5+ atom. In the third O2- site, O2- is bonded in a 4-coordinate geometry to one Li1+, two equivalent Cr2+, and one P5+ atom. In the fourth O2- site, O2- is bonded in a distorted tetrahedral geometry to three Li1+ and one P5+ atom. In the fifth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two Li1+, one Cr2+, and one P5+ atom. In the sixth O2- site, O2- is bonded in a rectangular see-saw-like geometry to three Li1+ and one P5+ atom. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a 1-coordinate geometry to three Li1+ and two equivalent Cr2+ atoms. In the second F1- site, F1- is bonded in a 6-coordinate geometry to four Li1+ and two equivalent Cr2+ atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-29. Materials Data on Li2CrPO4F by Materials Project. https://doi.org/10.17188/1300166

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↗