Search NASA⌕ Search

DOE OSTI · 1274952

Materials Data on K3Cu11Te16 by Materials Project

Abstract

K3Cu11Te16 crystallizes in the orthorhombic Imma space group. The structure is three-dimensional. there are two inequivalent K1+ sites. In the first K1+ site, K1+ is bonded in a 1-coordinate geometry to eight Te+0.88- atoms. There are a spread of K–Te bond distances ranging from 3.45–3.95 Å. In the second K1+ site, K1+ is bonded to twelve Te+0.88- atoms to form KTe12 cuboctahedra that share corners with fourteen CuTe4 tetrahedra, edges with two equivalent KTe12 cuboctahedra, and faces with eight CuTe4 tetrahedra. There are a spread of K–Te bond distances ranging from 3.68–3.85 Å. There are four inequivalent Cu1+ sites. In the first Cu1+ site, Cu1+ is bonded to four Te+0.88- atoms to form CuTe4 tetrahedra that share a cornercorner with one KTe12 cuboctahedra, corners with four CuTe4 tetrahedra, edges with two CuTe4 tetrahedra, and a faceface with one KTe12 cuboctahedra. There are a spread of Cu–Te bond distances ranging from 2.60–2.73 Å. In the second Cu1+ site, Cu1+ is bonded to four Te+0.88- atoms to form CuTe4 tetrahedra that share a cornercorner with one KTe12 cuboctahedra, corners with seven CuTe4 tetrahedra, an edgeedge with one CuTe4 tetrahedra, and a faceface with one KTe12 cuboctahedra. There are a spread of Cu–Te bond distances ranging from 2.58–2.65 Å. In the third Cu1+ site, Cu1+ is bonded to four Te+0.88- atoms to form CuTe4 tetrahedra that share corners with two equivalent KTe12 cuboctahedra and corners with four equivalent CuTe4 tetrahedra. All Cu–Te bond lengths are 2.61 Å. In the fourth Cu1+ site, Cu1+ is bonded to four Te+0.88- atoms to form distorted CuTe4 tetrahedra that share corners with two equivalent KTe12 cuboctahedra, corners with four equivalent CuTe4 tetrahedra, and edges with two equivalent CuTe4 tetrahedra. There are two shorter (2.59 Å) and two longer (2.60 Å) Cu–Te bond lengths. There are six inequivalent Te+0.88- sites. In the first Te+0.88- site, Te+0.88- is bonded in a 6-coordinate geometry to two equivalent K1+, three Cu1+, and one Te+0.88- atom. The Te–Te bond length is 2.89 Å. In the second Te+0.88- site, Te+0.88- is bonded in a distorted trigonal non-coplanar geometry to three K1+ and three Cu1+ atoms. In the third Te+0.88- site, Te+0.88- is bonded in a 7-coordinate geometry to two equivalent K1+, four Cu1+, and one Te+0.88- atom. The Te–Te bond length is 2.93 Å. In the fourth Te+0.88- site, Te+0.88- is bonded in a 3-coordinate geometry to one K1+ and three Cu1+ atoms. In the fifth Te+0.88- site, Te+0.88- is bonded in a 2-coordinate geometry to one K1+ and two equivalent Cu1+ atoms. In the sixth Te+0.88- site, Te+0.88- is bonded in a 2-coordinate geometry to two equivalent K1+, one Cu1+, and two equivalent Te+0.88- atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-05-02. Materials Data on K3Cu11Te16 by Materials Project. https://doi.org/10.17188/1274952

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↗