Search NASA⌕ Search

DOE OSTI · 1723633

Materials Data on LiMg by Materials Project

Abstract

LiMg crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are three inequivalent Li sites. In the first Li site, Li is bonded to six Li and six Mg atoms to form distorted LiLi6Mg6 cuboctahedra that share corners with six equivalent MgLi4Mg8 cuboctahedra, corners with twelve LiLi6Mg6 cuboctahedra, edges with three equivalent LiLi8Mg4 cuboctahedra, edges with fifteen MgLi4Mg8 cuboctahedra, faces with six LiLi6Mg6 cuboctahedra, and faces with eight MgLi4Mg8 cuboctahedra. There are four shorter (3.09 Å) and two longer (3.20 Å) Li–Li bond lengths. There are four shorter (3.08 Å) and two longer (3.09 Å) Li–Mg bond lengths. In the second Li site, Li is bonded to eight Li and four Mg atoms to form distorted LiLi8Mg4 cuboctahedra that share corners with six equivalent MgLi4Mg8 cuboctahedra, corners with twelve LiLi6Mg6 cuboctahedra, edges with three equivalent LiLi6Mg6 cuboctahedra, edges with eleven MgLi4Mg8 cuboctahedra, faces with six LiLi6Mg6 cuboctahedra, and faces with ten MgLi4Mg8 cuboctahedra. There are four shorter (3.10 Å) and two longer (3.20 Å) Li–Li bond lengths. There are two shorter (3.07 Å) and two longer (3.10 Å) Li–Mg bond lengths. In the third Li site, Li is bonded in a 12-coordinate geometry to six Li and four Mg atoms. There are two shorter (3.03 Å) and two longer (3.06 Å) Li–Mg bond lengths. There are three inequivalent Mg sites. In the first Mg site, Mg is bonded to four Li and eight Mg atoms to form distorted MgLi4Mg8 cuboctahedra that share corners with six equivalent MgLi4Mg8 cuboctahedra, corners with twelve LiLi6Mg6 cuboctahedra, edges with four equivalent MgLi4Mg8 cuboctahedra, edges with six LiLi6Mg6 cuboctahedra, faces with four LiLi6Mg6 cuboctahedra, and faces with fourteen MgLi4Mg8 cuboctahedra. There are a spread of Mg–Mg bond distances ranging from 3.12–3.20 Å. In the second Mg site, Mg is bonded to six Li and six Mg atoms to form distorted MgLi6Mg6 cuboctahedra that share corners with twelve MgLi4Mg8 cuboctahedra, edges with three equivalent MgLi4Mg8 cuboctahedra, edges with twelve LiLi8Mg4 cuboctahedra, faces with six LiLi6Mg6 cuboctahedra, and faces with twelve MgLi4Mg8 cuboctahedra. All Mg–Mg bond lengths are 3.20 Å. In the third Mg site, Mg is bonded to four Li and eight Mg atoms to form distorted MgLi4Mg8 cuboctahedra that share corners with twelve MgLi4Mg8 cuboctahedra, edges with seven MgLi4Mg8 cuboctahedra, edges with eight equivalent LiLi6Mg6 cuboctahedra, faces with eight LiLi6Mg6 cuboctahedra, and faces with ten MgLi4Mg8 cuboctahedra. Both Mg–Mg bond lengths are 3.20 Å.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-05-02. Materials Data on LiMg by Materials Project. https://doi.org/10.17188/1723633

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↗