Search NASA⌕ Search

DOE OSTI · 1280915

Materials Data on Os3C9Se2O9 by Materials Project

Abstract

Os3C9Se2O9 crystallizes in the triclinic P-1 space group. The structure is two-dimensional and consists of one Os3C9Se2O9 sheet oriented in the (0, 1, 0) direction. there are three inequivalent Os2- sites. In the first Os2- site, Os2- is bonded in a 5-coordinate geometry to three C+3.11+ and two Se2- atoms. All Os–C bond lengths are 1.91 Å. There are one shorter (2.58 Å) and one longer (2.60 Å) Os–Se bond lengths. In the second Os2- site, Os2- is bonded in a 5-coordinate geometry to three C+3.11+ and two Se2- atoms. There is one shorter (1.89 Å) and two longer (1.92 Å) Os–C bond length. There are one shorter (2.55 Å) and one longer (2.56 Å) Os–Se bond lengths. In the third Os2- site, Os2- is bonded in a 5-coordinate geometry to three C+3.11+ and two Se2- atoms. There is one shorter (1.88 Å) and two longer (1.92 Å) Os–C bond length. There are one shorter (2.55 Å) and one longer (2.57 Å) Os–Se bond lengths. There are nine inequivalent C+3.11+ sites. In the first C+3.11+ site, C+3.11+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the second C+3.11+ site, C+3.11+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the third C+3.11+ site, C+3.11+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the fourth C+3.11+ site, C+3.11+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the fifth C+3.11+ site, C+3.11+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.17 Å. In the sixth C+3.11+ site, C+3.11+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the seventh C+3.11+ site, C+3.11+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the eighth C+3.11+ site, C+3.11+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the ninth C+3.11+ site, C+3.11+ is bonded in a distorted linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. There are two inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a 4-coordinate geometry to three Os2- and four O2- atoms. There are a spread of Se–O bond distances ranging from 3.40–3.70 Å. In the second Se2- site, Se2- is bonded in a 5-coordinate geometry to three Os2- atoms. There are nine inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one C+3.11+ and one Se2- atom. In the second O2- site, O2- is bonded in a single-bond geometry to one C+3.11+ atom. In the third O2- site, O2- is bonded in a single-bond geometry to one C+3.11+ and one Se2- atom. In the fourth O2- site, O2- is bonded in a single-bond geometry to one C+3.11+ atom. In the fifth O2- site, O2- is bonded in a single-bond geometry to one C+3.11+ and one Se2- atom. In the sixth O2- site, O2- is bonded in a single-bond geometry to one C+3.11+ and one Se2- atom. In the seventh O2- site, O2- is bonded in a single-bond geometry to one C+3.11+ atom. In the eighth O2- site, O2- is bonded in a single-bond geometry to one C+3.11+ atom. In the ninth O2- site, O2- is bonded in a single-bond geometry to one C+3.11+ atom.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-05-02. Materials Data on Os3C9Se2O9 by Materials Project. https://doi.org/10.17188/1280915

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↗