Search NASA⌕ Search

DOE OSTI · 1753162

Materials Data on Cu6MoC20S4N5Cl9 by Materials Project

Abstract

MoCu6S4Cl9(C)5(C3N)5 crystallizes in the orthorhombic Cmc2_1 space group. The structure is zero-dimensional and consists of twenty 1-azatricyclo[1.1.0.0^{2,4}]butane molecules; twenty methane molecules; and four MoCu6S4Cl9 clusters. In each MoCu6S4Cl9 cluster, Mo2+ is bonded to four S2- atoms to form MoS4 tetrahedra that share an edgeedge with one CuS2Cl2 trigonal pyramid. There are three shorter (2.26 Å) and one longer (2.28 Å) Mo–S bond lengths. There are four inequivalent Cu1+ sites. In the first Cu1+ site, Cu1+ is bonded in a distorted rectangular see-saw-like geometry to two S2- and two Cl1- atoms. There are one shorter (2.41 Å) and one longer (2.43 Å) Cu–S bond lengths. There are one shorter (2.11 Å) and one longer (2.21 Å) Cu–Cl bond lengths. In the second Cu1+ site, Cu1+ is bonded to two equivalent S2- and two Cl1- atoms to form distorted CuS2Cl2 trigonal pyramids that share an edgeedge with one MoS4 tetrahedra. Both Cu–S bond lengths are 2.41 Å. There are one shorter (2.11 Å) and one longer (2.22 Å) Cu–Cl bond lengths. In the third Cu1+ site, Cu1+ is bonded in a 3-coordinate geometry to two S2- and three Cl1- atoms. There are one shorter (2.29 Å) and one longer (2.30 Å) Cu–S bond lengths. There are a spread of Cu–Cl bond distances ranging from 2.09–3.08 Å. In the fourth Cu1+ site, Cu1+ is bonded in a 3-coordinate geometry to two S2- and three Cl1- atoms. There are one shorter (2.29 Å) and one longer (2.30 Å) Cu–S bond lengths. There are one shorter (2.09 Å) and two longer (3.09 Å) Cu–Cl bond lengths. There are three inequivalent S2- sites. In the first S2- site, S2- is bonded in a distorted tetrahedral geometry to one Mo2+ and three Cu1+ atoms. In the second S2- site, S2- is bonded in a 4-coordinate geometry to one Mo2+ and three Cu1+ atoms. In the third S2- site, S2- is bonded in a 4-coordinate geometry to one Mo2+ and three Cu1+ atoms. There are six inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a single-bond geometry to one Cu1+ atom. In the second Cl1- site, Cl1- is bonded in a single-bond geometry to one Cu1+ atom. In the third Cl1- site, Cl1- is bonded in a single-bond geometry to one Cu1+ atom. In the fourth Cl1- site, Cl1- is bonded in a single-bond geometry to one Cu1+ atom. In the fifth Cl1- site, Cl1- is bonded in a distorted single-bond geometry to three Cu1+ atoms. In the sixth Cl1- site, Cl1- is bonded in a distorted single-bond geometry to three Cu1+ atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-05-02. Materials Data on Cu6MoC20S4N5Cl9 by Materials Project. https://doi.org/10.17188/1753162

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↗