Search NASA⌕ Search

DOE OSTI · 1263282

Materials Data on Li5P2N5 by Materials Project

Abstract

Li5P2N5 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are eight inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 3-coordinate geometry to three N3- atoms. There are two shorter (2.15 Å) and one longer (2.21 Å) Li–N bond lengths. In the second Li1+ site, Li1+ is bonded to four N3- atoms to form distorted LiN4 tetrahedra that share corners with four PN4 tetrahedra. There are a spread of Li–N bond distances ranging from 1.95–2.06 Å. In the third Li1+ site, Li1+ is bonded in a distorted trigonal planar geometry to three N3- atoms. There are one shorter (1.93 Å) and two longer (2.10 Å) Li–N bond lengths. In the fourth Li1+ site, Li1+ is bonded in a distorted trigonal planar geometry to three N3- atoms. There are a spread of Li–N bond distances ranging from 1.92–2.11 Å. In the fifth Li1+ site, Li1+ is bonded to six N3- atoms to form distorted LiN6 octahedra that share corners with six LiN6 octahedra and edges with six PN4 tetrahedra. The corner-sharing octahedral tilt angles are 18°. There are a spread of Li–N bond distances ranging from 2.22–2.26 Å. In the sixth Li1+ site, Li1+ is bonded to six N3- atoms to form distorted LiN6 octahedra that share corners with six LiN6 octahedra and edges with six PN4 tetrahedra. The corner-sharing octahedra tilt angles range from 17–18°. There are a spread of Li–N bond distances ranging from 2.18–2.22 Å. In the seventh Li1+ site, Li1+ is bonded in a distorted trigonal planar geometry to three N3- atoms. There is one shorter (1.90 Å) and two longer (2.08 Å) Li–N bond length. In the eighth Li1+ site, Li1+ is bonded in a distorted trigonal planar geometry to three N3- atoms. There are a spread of Li–N bond distances ranging from 1.92–2.13 Å. There are three inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four N3- atoms to form PN4 tetrahedra that share a cornercorner with one LiN4 tetrahedra, corners with three PN4 tetrahedra, and edges with three LiN6 octahedra. There are a spread of P–N bond distances ranging from 1.60–1.69 Å. In the second P5+ site, P5+ is bonded to four N3- atoms to form PN4 tetrahedra that share a cornercorner with one LiN4 tetrahedra, corners with three PN4 tetrahedra, and edges with three LiN6 octahedra. There are a spread of P–N bond distances ranging from 1.60–1.69 Å. In the third P5+ site, P5+ is bonded to four N3- atoms to form PN4 tetrahedra that share a cornercorner with one LiN4 tetrahedra, corners with three PN4 tetrahedra, and edges with three LiN6 octahedra. There is one shorter (1.61 Å) and three longer (1.68 Å) P–N bond length. There are seven inequivalent N3- sites. In the first N3- site, N3- is bonded to three Li1+ and two P5+ atoms to form a mixture of distorted edge and corner-sharing NLi3P2 trigonal bipyramids. In the second N3- site, N3- is bonded to three Li1+ and two P5+ atoms to form a mixture of distorted edge and corner-sharing NLi3P2 trigonal bipyramids. In the third N3- site, N3- is bonded to three Li1+ and two equivalent P5+ atoms to form a mixture of distorted edge and corner-sharing NLi3P2 trigonal bipyramids. In the fourth N3- site, N3- is bonded in a 6-coordinate geometry to five Li1+ and one P5+ atom. In the fifth N3- site, N3- is bonded to three Li1+ and two P5+ atoms to form a mixture of distorted edge and corner-sharing NLi3P2 trigonal bipyramids. In the sixth N3- site, N3- is bonded in a 6-coordinate geometry to five Li1+ and one P5+ atom. In the seventh N3- site, N3- is bonded in a 5-coordinate geometry to four Li1+ and one P5+ atom.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-05-29. Materials Data on Li5P2N5 by Materials Project. https://doi.org/10.17188/1263282

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↗