Search NASA⌕ Search

DOE OSTI · 1701649

Materials Data on Hf27(Si3P5)2 by Materials Project

Abstract

Hf27Si6P10 crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. there are nine inequivalent Hf sites. In the first Hf site, Hf is bonded in a distorted rectangular see-saw-like geometry to one Si and three P atoms. The Hf–Si bond length is 2.87 Å. There are a spread of Hf–P bond distances ranging from 2.69–2.77 Å. In the second Hf site, Hf is bonded in a 4-coordinate geometry to three Si and one P atom. There are two shorter (2.67 Å) and one longer (2.86 Å) Hf–Si bond lengths. The Hf–P bond length is 2.65 Å. In the third Hf site, Hf is bonded to two equivalent Si and three P atoms to form distorted HfSi2P3 trigonal bipyramids that share corners with two equivalent HfP6 pentagonal pyramids, corners with two equivalent HfSi2P3 trigonal bipyramids, an edgeedge with one HfP6 pentagonal pyramid, edges with two equivalent HfSi2P3 trigonal bipyramids, and a faceface with one HfSi2P3 trigonal bipyramid. Both Hf–Si bond lengths are 2.73 Å. There are one shorter (2.61 Å) and two longer (2.69 Å) Hf–P bond lengths. In the fourth Hf site, Hf is bonded in a 4-coordinate geometry to three equivalent Si and two equivalent P atoms. There are two shorter (2.75 Å) and one longer (3.10 Å) Hf–Si bond lengths. Both Hf–P bond lengths are 2.72 Å. In the fifth Hf site, Hf is bonded in a 4-coordinate geometry to three Si and two equivalent P atoms. There are two shorter (2.74 Å) and one longer (3.23 Å) Hf–Si bond lengths. Both Hf–P bond lengths are 2.70 Å. In the sixth Hf site, Hf is bonded in a 6-coordinate geometry to two equivalent Si and four equivalent P atoms. Both Hf–Si bond lengths are 2.79 Å. All Hf–P bond lengths are 2.75 Å. In the seventh Hf site, Hf is bonded to six P atoms to form a mixture of distorted face, edge, and corner-sharing HfP6 pentagonal pyramids. There are two shorter (2.68 Å) and four longer (2.75 Å) Hf–P bond lengths. In the eighth Hf site, Hf is bonded to six P atoms to form distorted HfP6 pentagonal pyramids that share corners with four equivalent HfP6 pentagonal pyramids, corners with four equivalent HfSi2P3 trigonal bipyramids, edges with four HfP6 pentagonal pyramids, edges with two equivalent HfSi2P3 trigonal bipyramids, and faces with three equivalent HfP6 pentagonal pyramids. There are two shorter (2.69 Å) and four longer (2.76 Å) Hf–P bond lengths. In the ninth Hf site, Hf is bonded in a distorted square co-planar geometry to two equivalent Si and two equivalent P atoms. Both Hf–Si bond lengths are 2.95 Å. Both Hf–P bond lengths are 2.68 Å. There are two inequivalent Si sites. In the first Si site, Si is bonded in a 9-coordinate geometry to nine Hf atoms. In the second Si site, Si is bonded in a 9-coordinate geometry to nine Hf atoms. There are four inequivalent P sites. In the first P site, P is bonded in a 8-coordinate geometry to eight Hf atoms. In the second P site, P is bonded in a 8-coordinate geometry to eight Hf atoms. In the third P site, P is bonded in a 8-coordinate geometry to eight Hf atoms. In the fourth P site, P is bonded to seven Hf atoms to form a mixture of distorted edge and corner-sharing PHf7 pentagonal bipyramids.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-29. Materials Data on Hf27(Si3P5)2 by Materials Project. https://doi.org/10.17188/1701649

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↗