Search NASA⌕ Search

DOE OSTI · 1293048

Materials Data on Li4(NiO2)5 by Materials Project

Abstract

Li4(NiO2)5 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 1.93–2.12 Å. In the second Li1+ site, Li1+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 1.92–2.03 Å. In the third Li1+ site, Li1+ is bonded in a distorted rectangular see-saw-like geometry to five O2- atoms. There are a spread of Li–O bond distances ranging from 1.93–2.67 Å. In the fourth Li1+ site, Li1+ is bonded in a distorted rectangular see-saw-like geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 1.93–2.12 Å. There are five inequivalent Ni+3.20+ sites. In the first Ni+3.20+ site, Ni+3.20+ is bonded to six O2- atoms to form edge-sharing NiO6 octahedra. There are a spread of Ni–O bond distances ranging from 1.87–2.09 Å. In the second Ni+3.20+ site, Ni+3.20+ is bonded to six O2- atoms to form edge-sharing NiO6 octahedra. There are a spread of Ni–O bond distances ranging from 1.89–2.18 Å. In the third Ni+3.20+ site, Ni+3.20+ is bonded to six O2- atoms to form edge-sharing NiO6 octahedra. There are a spread of Ni–O bond distances ranging from 1.89–2.11 Å. In the fourth Ni+3.20+ site, Ni+3.20+ is bonded to six O2- atoms to form edge-sharing NiO6 octahedra. There are a spread of Ni–O bond distances ranging from 1.89–2.17 Å. In the fifth Ni+3.20+ site, Ni+3.20+ is bonded to six O2- atoms to form edge-sharing NiO6 octahedra. There are a spread of Ni–O bond distances ranging from 1.87–1.91 Å. There are ten inequivalent O2- sites. In the first O2- site, O2- is bonded to two Li1+ and three Ni+3.20+ atoms to form OLi2Ni3 trigonal bipyramids that share corners with four OLi2Ni3 square pyramids, corners with two equivalent OLiNi3 tetrahedra, a cornercorner with one OLi2Ni3 trigonal bipyramid, edges with two OLi2Ni3 square pyramids, edges with two equivalent OLi2Ni3 trigonal bipyramids, and an edgeedge with one OLiNi3 trigonal pyramid. In the second O2- site, O2- is bonded to two Li1+ and three Ni+3.20+ atoms to form OLi2Ni3 square pyramids that share corners with two OLi2Ni3 square pyramids, a cornercorner with one OLiNi3 tetrahedra, corners with two OLi2Ni3 trigonal bipyramids, corners with two equivalent OLiNi3 trigonal pyramids, edges with two OLi2Ni3 trigonal bipyramids, and an edgeedge with one OLiNi3 trigonal pyramid. In the third O2- site, O2- is bonded in a 6-coordinate geometry to three Li1+ and three Ni+3.20+ atoms. In the fourth O2- site, O2- is bonded to two Li1+ and three Ni+3.20+ atoms to form OLi2Ni3 trigonal bipyramids that share corners with two OLi2Ni3 square pyramids, a cornercorner with one OLi2Ni3 trigonal bipyramid, corners with two equivalent OLiNi3 trigonal pyramids, edges with three OLi2Ni3 square pyramids, an edgeedge with one OLiNi3 tetrahedra, and edges with two equivalent OLi2Ni3 trigonal bipyramids. In the fifth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+ and three Ni+3.20+ atoms. In the sixth O2- site, O2- is bonded to one Li1+ and three Ni+3.20+ atoms to form distorted OLiNi3 trigonal pyramids that share corners with four OLi2Ni3 square pyramids, a cornercorner with one OLiNi3 tetrahedra, corners with two equivalent OLi2Ni3 trigonal bipyramids, an edgeedge with one OLi2Ni3 square pyramid, and an edgeedge with one OLi2Ni3 trigonal bipyramid. In the seventh O2- site, O2- is bonded to one Li1+ and three Ni+3.20+ atoms to form distorted OLiNi3 tetrahedra that share corners with four OLi2Ni3 square pyramids, corners with two equivalent OLi2Ni3 trigonal bipyramids, a cornercorner with one OLiNi3 trigonal pyramid, edges with two OLi2Ni3 square pyramids, and an edgeedge with one OLi2Ni3 trigonal bipyramid. In the eighth O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+ and three Ni+3.20+ atoms. In the ninth O2- site, O2- is bonded to two Li1+ and three Ni+3.20+ atoms to form distorted OLi2Ni3 square pyramids that share a cornercorner with one OLi2Ni3 square pyramid, a cornercorner with one OLiNi3 tetrahedra, corners with two equivalent OLi2Ni3 trigonal bipyramids, a cornercorner with one OLiNi3 trigonal pyramid, edges with two equivalent OLi2Ni3 square pyramids, an edgeedge with one OLiNi3 tetrahedra, and an edgeedge with one OLi2Ni3 trigonal bipyramid. In the tenth O2- site, O2- is bonded to two Li1+ and three Ni+3.20+ atoms to form OLi2Ni3 square pyramids that share a cornercorner with one OLi2Ni3 square pyramid, corners with two equivalent OLiNi3 tetrahedra, corners with two OLi2Ni3 trigonal bipyramids, a cornercorner with one OLiNi3 trigonal pyramid, edges with two equivalent OLi2Ni3 square pyramids, an edgeedge with one OLiNi3 tetrahedra, and edges with two OLi2Ni3 trigonal bipyramids.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-30. Materials Data on Li4(NiO2)5 by Materials Project. https://doi.org/10.17188/1293048

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↗