Search NASA⌕ Search

DOE OSTI · 1204407

Materials Data on RbLi7Ge8 by Materials Project

Abstract

RbLi7Ge8 crystallizes in the hexagonal P6_3mc space group. The structure is three-dimensional. there are two inequivalent Rb sites. In the first Rb site, Rb is bonded in a 10-coordinate geometry to six Li and seven Ge atoms. There are three shorter (3.58 Å) and three longer (3.90 Å) Rb–Li bond lengths. There are one shorter (3.74 Å) and six longer (3.87 Å) Rb–Ge bond lengths. In the second Rb site, Rb is bonded in a 12-coordinate geometry to six Li and twelve Ge atoms. There are three shorter (3.56 Å) and three longer (3.63 Å) Rb–Li bond lengths. There are a spread of Rb–Ge bond distances ranging from 3.67–3.75 Å. There are six inequivalent Li sites. In the first Li site, Li is bonded in a distorted trigonal non-coplanar geometry to one Rb and three Ge atoms. There are one shorter (2.56 Å) and two longer (2.69 Å) Li–Ge bond lengths. In the second Li site, Li is bonded in a distorted trigonal non-coplanar geometry to two Rb and five Ge atoms. There are a spread of Li–Ge bond distances ranging from 2.64–3.12 Å. In the third Li site, Li is bonded in a 6-coordinate geometry to one Rb and six Ge atoms. There are a spread of Li–Ge bond distances ranging from 2.77–2.87 Å. In the fourth Li site, Li is bonded in a 9-coordinate geometry to one Li and nine Ge atoms. The Li–Li bond length is 3.01 Å. There are a spread of Li–Ge bond distances ranging from 2.85–3.07 Å. In the fifth Li site, Li is bonded in a 9-coordinate geometry to one Li and nine Ge atoms. The Li–Li bond length is 3.01 Å. There are six shorter (2.91 Å) and three longer (3.04 Å) Li–Ge bond lengths. In the sixth Li site, Li is bonded in a 12-coordinate geometry to four Li and twelve Ge atoms. There are a spread of Li–Ge bond distances ranging from 2.99–3.10 Å. There are five inequivalent Ge sites. In the first Ge site, Ge is bonded in a 6-coordinate geometry to one Rb, six Li, and three equivalent Ge atoms. All Ge–Ge bond lengths are 2.62 Å. In the second Ge site, Ge is bonded in a 1-coordinate geometry to one Rb, five Li, and three Ge atoms. Both Ge–Ge bond lengths are 2.58 Å. In the third Ge site, Ge is bonded in a 11-coordinate geometry to one Rb, seven Li, and three Ge atoms. There are one shorter (2.55 Å) and two longer (2.66 Å) Ge–Ge bond lengths. In the fourth Ge site, Ge is bonded in a 10-coordinate geometry to two Rb, five Li, and three Ge atoms. There are one shorter (2.53 Å) and one longer (2.62 Å) Ge–Ge bond lengths. In the fifth Ge site, Ge is bonded in a 9-coordinate geometry to six Li and three Ge atoms. Both Ge–Ge bond lengths are 2.69 Å.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-30. Materials Data on RbLi7Ge8 by Materials Project. https://doi.org/10.17188/1204407

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↗