Search NASA⌕ Search

DOE OSTI · 1688960

Materials Data on Rb2Fe5F17 by Materials Project

Abstract

Rb2Fe5F17 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are three inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded in a distorted hexagonal planar geometry to six F1- atoms. There are a spread of Rb–F bond distances ranging from 2.89–3.11 Å. In the second Rb1+ site, Rb1+ is bonded in a 9-coordinate geometry to nine F1- atoms. There are a spread of Rb–F bond distances ranging from 2.69–3.52 Å. In the third Rb1+ site, Rb1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Rb–F bond distances ranging from 2.78–2.91 Å. There are six inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded in a distorted body-centered cubic geometry to eight F1- atoms. There are a spread of Fe–F bond distances ranging from 2.09–2.52 Å. In the second Fe3+ site, Fe3+ is bonded to six F1- atoms to form distorted FeF6 octahedra that share a cornercorner with one FeF5 square pyramid, a cornercorner with one FeF5 trigonal bipyramid, and an edgeedge with one FeF7 pentagonal bipyramid. There are a spread of Fe–F bond distances ranging from 1.84–2.12 Å. In the third Fe3+ site, Fe3+ is bonded to seven F1- atoms to form distorted FeF7 pentagonal bipyramids that share a cornercorner with one FeF5 trigonal bipyramid, edges with two FeF6 octahedra, and an edgeedge with one FeF7 pentagonal bipyramid. There are a spread of Fe–F bond distances ranging from 1.95–2.23 Å. In the fourth Fe3+ site, Fe3+ is bonded to five F1- atoms to form distorted FeF5 trigonal bipyramids that share a cornercorner with one FeF6 octahedra, a cornercorner with one FeF7 pentagonal bipyramid, and a cornercorner with one FeF5 square pyramid. The corner-sharing octahedral tilt angles are 18°. There are a spread of Fe–F bond distances ranging from 1.80–1.98 Å. In the fifth Fe3+ site, Fe3+ is bonded to five F1- atoms to form distorted FeF5 square pyramids that share corners with two FeF6 octahedra and a cornercorner with one FeF5 trigonal bipyramid. The corner-sharing octahedra tilt angles range from 15–25°. There are a spread of Fe–F bond distances ranging from 1.82–2.00 Å. In the sixth Fe3+ site, Fe3+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with two equivalent FeF5 square pyramids and edges with two equivalent FeF7 pentagonal bipyramids. There is four shorter (1.96 Å) and two longer (1.99 Å) Fe–F bond length. There are seventeen inequivalent F1- sites. In the first F1- site, F1- is bonded in a 2-coordinate geometry to two equivalent Rb1+ and one F1- atom. The F–F bond length is 2.05 Å. In the second F1- site, F1- is bonded in a 2-coordinate geometry to three Fe3+ atoms. In the third F1- site, F1- is bonded in a distorted single-bond geometry to one Rb1+ and one Fe3+ atom. In the fourth F1- site, F1- is bonded in a single-bond geometry to one Rb1+ and one Fe3+ atom. In the fifth F1- site, F1- is bonded in a bent 150 degrees geometry to two Fe3+ atoms. In the sixth F1- site, F1- is bonded in a distorted single-bond geometry to three Rb1+ and one Fe3+ atom. In the seventh F1- site, F1- is bonded in a 2-coordinate geometry to one Rb1+ and two Fe3+ atoms. In the eighth F1- site, F1- is bonded in a linear geometry to two Fe3+ atoms. In the ninth F1- site, F1- is bonded in a 3-coordinate geometry to one Rb1+ and two Fe3+ atoms. In the tenth F1- site, F1- is bonded in a trigonal non-coplanar geometry to three Fe3+ atoms. In the eleventh F1- site, F1- is bonded in a 1-coordinate geometry to three Rb1+ and one Fe3+ atom. In the twelfth F1- site, F1- is bonded in a distorted single-bond geometry to two Rb1+ and one Fe3+ atom. In the thirteenth F1- site, F1- is bonded in a water-like geometry to two equivalent Fe3+ atoms. In the fourteenth F1- site, F1- is bonded in a bent 150 degrees geometry to two Fe3+ atoms. In the fifteenth F1- site, F1- is bonded in a linear geometry to two Fe3+ atoms. In the sixteenth F1- site, F1- is bonded in a distorted water-like geometry to one Rb1+ and two Fe3+ atoms. In the seventeenth F1- site, F1- is bonded in a 3-coordinate geometry to three Fe3+ atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2019-01-11. Materials Data on Rb2Fe5F17 by Materials Project. https://doi.org/10.17188/1688960

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↗