Search NASA⌕ Search

DOE OSTI · 1276962

Materials Data on Ce4Al23Ni6 by Materials Project

Abstract

Ce4Ni6Al23 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Ce sites. In the first Ce site, Ce is bonded in a 11-coordinate geometry to two equivalent Ni and thirteen Al atoms. Both Ce–Ni bond lengths are 3.26 Å. There are a spread of Ce–Al bond distances ranging from 3.06–3.41 Å. In the second Ce site, Ce is bonded in a 11-coordinate geometry to two equivalent Ni and thirteen Al atoms. Both Ce–Ni bond lengths are 3.29 Å. There are a spread of Ce–Al bond distances ranging from 3.07–3.38 Å. There are three inequivalent Ni sites. In the first Ni site, Ni is bonded in a 7-coordinate geometry to two equivalent Ce and seven Al atoms. There are a spread of Ni–Al bond distances ranging from 2.37–2.53 Å. In the second Ni site, Ni is bonded in a 7-coordinate geometry to nine Al atoms. There are a spread of Ni–Al bond distances ranging from 2.42–2.81 Å. In the third Ni site, Ni is bonded in a 10-coordinate geometry to two equivalent Ce and eight Al atoms. There are a spread of Ni–Al bond distances ranging from 2.39–2.55 Å. There are twelve inequivalent Al sites. In the first Al site, Al is bonded in a distorted bent 150 degrees geometry to two equivalent Ce, two Ni, and five Al atoms. There are a spread of Al–Al bond distances ranging from 2.72–2.89 Å. In the second Al site, Al is bonded in a distorted trigonal planar geometry to three Ni and two Al atoms. There are one shorter (2.72 Å) and one longer (2.73 Å) Al–Al bond lengths. In the third Al site, Al is bonded in a 12-coordinate geometry to four Ce and eight Al atoms. There are a spread of Al–Al bond distances ranging from 2.88–3.19 Å. In the fourth Al site, Al is bonded to two Ce, two equivalent Ni, and eight Al atoms to form distorted face-sharing AlCe2Al8Ni2 cuboctahedra. There are two shorter (2.74 Å) and one longer (2.84 Å) Al–Al bond lengths. In the fifth Al site, Al is bonded in a 3-coordinate geometry to one Ce, three equivalent Ni, and six Al atoms. There are two shorter (2.62 Å) and one longer (2.66 Å) Al–Al bond lengths. In the sixth Al site, Al is bonded in a 3-coordinate geometry to three equivalent Ce and three equivalent Ni atoms. In the seventh Al site, Al is bonded in a distorted bent 150 degrees geometry to three Ce, two Ni, and three Al atoms. In the eighth Al site, Al is bonded in a distorted single-bond geometry to three Ce, one Ni, and four Al atoms. Both Al–Al bond lengths are 2.91 Å. In the ninth Al site, Al is bonded in a 3-coordinate geometry to two equivalent Ce, three Ni, and one Al atom. In the tenth Al site, Al is bonded in a 2-coordinate geometry to three Ce, two equivalent Ni, and one Al atom. In the eleventh Al site, Al is bonded in a 12-coordinate geometry to four equivalent Ce and six Al atoms. In the twelfth Al site, Al is bonded in a distorted trigonal non-coplanar geometry to one Ce, three Ni, and one Al atom.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-07-22. Materials Data on Ce4Al23Ni6 by Materials Project. https://doi.org/10.17188/1276962

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↗