Search NASA⌕ Search

DOE OSTI · 1279820

Materials Data on Co7Te4(BrO2)6 by Materials Project

Abstract

Co7(TeO3)4Br6 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are fourteen inequivalent Co2+ sites. In the first Co2+ site, Co2+ is bonded in a 4-coordinate geometry to four O2- and one Br1- atom. There are a spread of Co–O bond distances ranging from 2.06–2.11 Å. The Co–Br bond length is 2.66 Å. In the second Co2+ site, Co2+ is bonded to four O2- and two Br1- atoms to form distorted CoBr2O4 octahedra that share a cornercorner with one CoBr4O2 octahedra and an edgeedge with one CoBr2O4 octahedra. The corner-sharing octahedral tilt angles are 15°. There are a spread of Co–O bond distances ranging from 2.00–2.13 Å. There are one shorter (2.57 Å) and one longer (2.80 Å) Co–Br bond lengths. In the third Co2+ site, Co2+ is bonded in a 4-coordinate geometry to four O2- and one Br1- atom. There are a spread of Co–O bond distances ranging from 2.06–2.11 Å. The Co–Br bond length is 2.66 Å. In the fourth Co2+ site, Co2+ is bonded to four O2- and two Br1- atoms to form distorted edge-sharing CoBr2O4 octahedra. There are a spread of Co–O bond distances ranging from 2.00–2.13 Å. There are one shorter (2.57 Å) and one longer (2.82 Å) Co–Br bond lengths. In the fifth Co2+ site, Co2+ is bonded to four O2- and two Br1- atoms to form distorted CoBr2O4 octahedra that share a cornercorner with one CoBr4O2 octahedra and an edgeedge with one CoBr2O4 octahedra. The corner-sharing octahedral tilt angles are 16°. There are a spread of Co–O bond distances ranging from 2.01–2.13 Å. There are one shorter (2.56 Å) and one longer (2.81 Å) Co–Br bond lengths. In the sixth Co2+ site, Co2+ is bonded in a 6-coordinate geometry to four O2- and two Br1- atoms. There are a spread of Co–O bond distances ranging from 1.98–2.26 Å. There are one shorter (2.58 Å) and one longer (3.03 Å) Co–Br bond lengths. In the seventh Co2+ site, Co2+ is bonded to two O2- and four Br1- atoms to form distorted corner-sharing CoBr4O2 octahedra. The corner-sharing octahedra tilt angles range from 15–16°. Both Co–O bond lengths are 1.96 Å. There are a spread of Co–Br bond distances ranging from 2.70–2.77 Å. In the eighth Co2+ site, Co2+ is bonded in a 4-coordinate geometry to four O2- and one Br1- atom. There are a spread of Co–O bond distances ranging from 2.06–2.11 Å. The Co–Br bond length is 2.65 Å. In the ninth Co2+ site, Co2+ is bonded in a 6-coordinate geometry to four O2- and two Br1- atoms. There are a spread of Co–O bond distances ranging from 1.98–2.26 Å. There are one shorter (2.57 Å) and one longer (3.08 Å) Co–Br bond lengths. In the tenth Co2+ site, Co2+ is bonded in a 6-coordinate geometry to four O2- and two Br1- atoms. There are a spread of Co–O bond distances ranging from 1.98–2.26 Å. There are one shorter (2.58 Å) and one longer (3.03 Å) Co–Br bond lengths. In the eleventh Co2+ site, Co2+ is bonded in a distorted linear geometry to two O2- and four Br1- atoms. Both Co–O bond lengths are 1.96 Å. There are a spread of Co–Br bond distances ranging from 2.70–2.80 Å. In the twelfth Co2+ site, Co2+ is bonded in a 4-coordinate geometry to four O2- and one Br1- atom. There are a spread of Co–O bond distances ranging from 2.06–2.11 Å. The Co–Br bond length is 2.67 Å. In the thirteenth Co2+ site, Co2+ is bonded to four O2- and two Br1- atoms to form distorted edge-sharing CoBr2O4 octahedra. There are a spread of Co–O bond distances ranging from 2.00–2.13 Å. There are one shorter (2.57 Å) and one longer (2.82 Å) Co–Br bond lengths. In the fourteenth Co2+ site, Co2+ is bonded in a 6-coordinate geometry to four O2- and two Br1- atoms. There are a spread of Co–O bond distances ranging from 1.98–2.26 Å. There are one shorter (2.58 Å) and one longer (3.06 Å) Co–Br bond lengths. There are eight inequivalent Te4+ sites. In the first Te4+ site, Te4+ is bonded in a 3-coordinate geometry to three O2- and one Br1- atom. There are a spread of Te–O bond distances ranging from 1.90–2.00 Å. The Te–Br bond length is 3.47 Å. In the second Te4+ site, Te4+ is bonded in a 3-coordinate geometry to three O2- and one Br1- atom. There are a spread of Te–O bond distances ranging from 1.88–1.92 Å. The Te–Br bond length is 3.47 Å. In the third Te4+ site, Te4+ is bonded in a 3-coordinate geometry to three O2- atoms. There are a spread of Te–O bond distances ranging from 1.90–2.00 Å. In the fourth Te4+ site, Te4+ is bonded in a 3-coordinate geometry to three O2- and one Br1- atom. There are a spread of Te–O bond distances ranging from 1.90–2.00 Å. The Te–Br bond length is 3.48 Å. In the fifth Te4+ site, Te4+ is bonded in a 3-coordinate geometry to three O2- and one Br1- atom. There are a spread of Te–O bond distances ranging from 1.88–1.92 Å. The Te–Br bond length is 3.46 Å. In the sixth Te4+ site, Te4+ is bonded in a 3-coordinate geometry to three O2- atoms. There are a spread of Te–O bond distances ranging from 1.88–1.92 Å. In the seventh Te4+ site, Te4+ is bonded in a 3-coordinate geometry to three O2- atoms. There are a spread of Te–O bond distances ranging from 1.88–1.92 Å. In the eighth Te4+ site, Te4+ is bonded in a 3-coordinate geometry to three O2- atoms. There are a spread of Te–O bond distances ranging from 1.90–2.00 Å. There are twenty-four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the sixth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the seventh O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the eighth O2- site, O2- is bonded in a distorted trigonal pyramidal geometry to three Co2+ and one Te4+ atom. In the ninth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the tenth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the eleventh O2- site, O2- is bonded in a trigonal non-coplanar geometry to two Co2+ and one Te4+ atom. In the twelfth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the thirteenth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the fourteenth O2- site, O2- is bonded in a trigonal non-coplanar geometry to two Co2+ and one Te4+ atom. In the fifteenth O2- site, O2- is bonded in a trigonal non-coplanar geometry to two Co2+ and one Te4+ atom. In the sixteenth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the seventeenth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the eighteenth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the nineteenth O2- site, O2- is bonded in a trigonal non-coplanar geometry to two Co2+ and one Te4+ atom. In the twentieth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. In the twenty-first O2- site, O2- is bonded in a distorted trigonal pyramidal geometry to three Co2+ and one Te4+ atom. In the twenty-second O2- site, O2- is bonded in a distorted trigonal pyramidal geometry to three Co2+ and one Te4+ atom. In the twenty-third O2- site, O2- is bonded in a distorted trigonal pyramidal geometry to three Co2+ and one Te4+ atom. In the twenty-fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co2+ and one Te4+ atom. There are twelve inequivalent Br1- sites. In the first Br1- site, Br1- is bonded in a 2-coordinate geometry to three Co2+ and two Te4+ atoms. In the second Br1- site, Br1- is bonded in a 2-coordinate geometry to three Co2+ and two Te4+ atoms. In the third Br1- site, Br1- is bonded in a 2-coordinate geometry to three Co2+ atoms. In the fourth Br1- site, Br1- is bonded in a 2-coordinate geometry to two Co2+ atoms. In the fifth Br1- site, Br1- is bonded in a 1-coordinate geometry to two Co2+ atoms. In the sixth Br1- site, Br1- is bonded in a 1-coordinate geometry to two Co2+ atoms. In the seventh Br1- site, Br1- is bonded in a 2-coordinate geometry to two Co2+ atoms. In the eighth Br1- site, Br1- is bonded in a 1-coordinate geometry to two Co2+ atoms. In the ninth Br1- site, Br1- is bonded in a 2-coordinate geometry to three Co2+ atoms. In the tenth Br1- site, Br1- is bonded in a 2-coordinate geometry to two Co2+ atoms. In the eleventh Br1- site, Br1- is bonded in a 1-coordinate geometry to two Co2+ atoms. In the twelfth Br1- site, Br1- is bonded in a 2-coordinate geometry to two Co2+ atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-08-03. Materials Data on Co7Te4(BrO2)6 by Materials Project. https://doi.org/10.17188/1279820

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↗