Search NASA⌕ Search

DOE OSTI · 1665344

Materials Data on Dy3C4 by Materials Project

Abstract

Dy3C4 crystallizes in the tetragonal P4/mnc space group. The structure is three-dimensional. there are four inequivalent Dy3+ sites. In the first Dy3+ site, Dy3+ is bonded in a 7-coordinate geometry to seven C+2.25- atoms. There are a spread of Dy–C bond distances ranging from 2.35–2.85 Å. In the second Dy3+ site, Dy3+ is bonded to seven C+2.25- atoms to form distorted DyC7 pentagonal bipyramids that share a cornercorner with one DyC6 octahedra, corners with two equivalent DyC7 pentagonal bipyramids, edges with three DyC6 octahedra, edges with two equivalent DyC7 pentagonal bipyramids, and faces with two equivalent DyC7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 1°. There are a spread of Dy–C bond distances ranging from 2.50–2.76 Å. In the third Dy3+ site, Dy3+ is bonded to six C+2.25- atoms to form DyC6 octahedra that share corners with two equivalent DyC6 octahedra, corners with four equivalent DyC7 pentagonal bipyramids, and edges with four equivalent DyC7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 0°. There are two shorter (2.50 Å) and four longer (2.61 Å) Dy–C bond lengths. In the fourth Dy3+ site, Dy3+ is bonded to six C+2.25- atoms to form DyC6 octahedra that share a cornercorner with one DyC6 octahedra and edges with four equivalent DyC7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 0°. There are a spread of Dy–C bond distances ranging from 2.34–2.64 Å. There are seven inequivalent C+2.25- sites. In the first C+2.25- site, C+2.25- is bonded to six Dy3+ atoms to form a mixture of edge and corner-sharing CDy6 octahedra. The corner-sharing octahedra tilt angles range from 0–85°. In the second C+2.25- site, C+2.25- is bonded in a 2-coordinate geometry to four equivalent Dy3+ and two equivalent C+2.25- atoms. Both C–C bond lengths are 1.35 Å. In the third C+2.25- site, C+2.25- is bonded to six Dy3+ atoms to form a mixture of edge and corner-sharing CDy6 octahedra. The corner-sharing octahedral tilt angles are 0°. In the fourth C+2.25- site, C+2.25- is bonded to six Dy3+ atoms to form a mixture of edge and corner-sharing CDy6 octahedra. The corner-sharing octahedral tilt angles are 0°. Both C–Dy bond lengths are 2.35 Å. In the fifth C+2.25- site, C+2.25- is bonded to six Dy3+ atoms to form a mixture of edge and corner-sharing CDy6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are a spread of C–Dy bond distances ranging from 2.35–2.64 Å. In the sixth C+2.25- site, C+2.25- is bonded in a 6-coordinate geometry to five Dy3+ and one C+2.25- atom. The C–C bond length is 1.31 Å. In the seventh C+2.25- site, C+2.25- is bonded to five Dy3+ and one C+2.25- atom to form a mixture of edge and corner-sharing CDy5C octahedra. The corner-sharing octahedra tilt angles range from 4–85°.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-30. Materials Data on Dy3C4 by Materials Project. https://doi.org/10.17188/1665344

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↗