Search NASA⌕ Search

DOE OSTI · 1655943

Materials Data on Nd2Co17N2 by Materials Project

Abstract

Nd2Co17N2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Nd is bonded in a distorted bent 120 degrees geometry to nine Co and two equivalent N atoms. There are a spread of Nd–Co bond distances ranging from 2.99–3.41 Å. Both Nd–N bond lengths are 2.51 Å. There are seven inequivalent Co sites. In the first Co site, Co is bonded in a 2-coordinate geometry to one Nd and thirteen Co atoms. There are a spread of Co–Co bond distances ranging from 2.32–2.74 Å. In the second Co site, Co is bonded to three equivalent Nd and nine Co atoms to form distorted CoNd3Co9 cuboctahedra that share corners with eleven CoNd3Co9 cuboctahedra, corners with four equivalent NNd2Co4 octahedra, edges with four CoNd3Co9 cuboctahedra, faces with eight CoNd3Co9 cuboctahedra, and faces with two equivalent NNd2Co4 octahedra. The corner-sharing octahedra tilt angles range from 62–69°. There are a spread of Co–Co bond distances ranging from 2.42–2.62 Å. In the third Co site, Co is bonded in a single-bond geometry to five Co and one N atom. There are a spread of Co–Co bond distances ranging from 2.42–2.56 Å. The Co–N bond length is 1.83 Å. In the fourth Co site, Co is bonded to two equivalent Nd and ten Co atoms to form distorted CoNd2Co10 cuboctahedra that share corners with eight CoNd3Co9 cuboctahedra, corners with four equivalent NNd2Co4 octahedra, edges with three CoNd2Co10 cuboctahedra, edges with two equivalent NNd2Co4 octahedra, and faces with nine CoNd3Co9 cuboctahedra. The corner-sharing octahedra tilt angles range from 21–29°. There are two shorter (2.38 Å) and two longer (2.41 Å) Co–Co bond lengths. In the fifth Co site, Co is bonded in a single-bond geometry to six Co and one N atom. There are one shorter (2.37 Å) and one longer (2.41 Å) Co–Co bond lengths. The Co–N bond length is 1.88 Å. In the sixth Co site, Co is bonded to two equivalent Nd and ten Co atoms to form distorted CoNd2Co10 cuboctahedra that share corners with fourteen CoNd3Co9 cuboctahedra, edges with two equivalent CoNd3Co9 cuboctahedra, faces with ten CoNd3Co9 cuboctahedra, and faces with four equivalent NNd2Co4 octahedra. In the seventh Co site, Co is bonded to two equivalent Nd and ten Co atoms to form distorted CoNd2Co10 cuboctahedra that share corners with eight CoNd3Co9 cuboctahedra, corners with two equivalent NNd2Co4 octahedra, edges with four CoNd2Co10 cuboctahedra, faces with eight CoNd3Co9 cuboctahedra, and faces with two equivalent NNd2Co4 octahedra. The corner-sharing octahedral tilt angles are 45°. N is bonded to two equivalent Nd and four Co atoms to form NNd2Co4 octahedra that share corners with ten CoNd3Co9 cuboctahedra, corners with two equivalent NNd2Co4 octahedra, edges with two equivalent CoNd2Co10 cuboctahedra, and faces with six CoNd2Co10 cuboctahedra. The corner-sharing octahedral tilt angles are 63°.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-07-15. Materials Data on Nd2Co17N2 by Materials Project. https://doi.org/10.17188/1655943

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↗