Search NASA⌕ Search

DOE OSTI · 1750638

Materials Data on Rb2Ag2Sn(PSe3)3 by Materials Project

Abstract

Rb2Ag2Sn(PSe3)3 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded in a 9-coordinate geometry to nine Se2- atoms. There are a spread of Rb–Se bond distances ranging from 3.59–3.82 Å. In the second Rb1+ site, Rb1+ is bonded in a 9-coordinate geometry to nine Se2- atoms. There are a spread of Rb–Se bond distances ranging from 3.51–3.93 Å. There are two inequivalent Ag+1.50+ sites. In the first Ag+1.50+ site, Ag+1.50+ is bonded in a 3-coordinate geometry to three Se2- atoms. There are a spread of Ag–Se bond distances ranging from 2.63–2.69 Å. In the second Ag+1.50+ site, Ag+1.50+ is bonded in a distorted trigonal non-coplanar geometry to three Se2- atoms. There are a spread of Ag–Se bond distances ranging from 2.65–2.72 Å. Sn4+ is bonded in a distorted T-shaped geometry to three Se2- atoms. There are a spread of Sn–Se bond distances ranging from 2.75–2.84 Å. There are three inequivalent P3+ sites. In the first P3+ site, P3+ is bonded in a trigonal non-coplanar geometry to three Se2- atoms. There are a spread of P–Se bond distances ranging from 2.15–2.26 Å. In the second P3+ site, P3+ is bonded in a trigonal non-coplanar geometry to three Se2- atoms. There are one shorter (2.19 Å) and two longer (2.25 Å) P–Se bond lengths. In the third P3+ site, P3+ is bonded in a trigonal non-coplanar geometry to three Se2- atoms. There are a spread of P–Se bond distances ranging from 2.19–2.26 Å. There are nine inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a 1-coordinate geometry to three Rb1+ and one P3+ atom. In the second Se2- site, Se2- is bonded in a 4-coordinate geometry to two Rb1+, one Sn4+, and one P3+ atom. In the third Se2- site, Se2- is bonded in a 4-coordinate geometry to two equivalent Rb1+, one Sn4+, and one P3+ atom. In the fourth Se2- site, Se2- is bonded in a 4-coordinate geometry to two equivalent Rb1+, one Ag+1.50+, and one P3+ atom. In the fifth Se2- site, Se2- is bonded in a 2-coordinate geometry to two equivalent Rb1+, one Ag+1.50+, and one P3+ atom. In the sixth Se2- site, Se2- is bonded to two equivalent Rb1+, one Ag+1.50+, and one P3+ atom to form distorted edge-sharing SeRb2AgP trigonal pyramids. In the seventh Se2- site, Se2- is bonded in a 3-coordinate geometry to one Rb1+, two equivalent Ag+1.50+, and one P3+ atom. In the eighth Se2- site, Se2- is bonded in a 4-coordinate geometry to two Rb1+, one Sn4+, and one P3+ atom. In the ninth Se2- site, Se2- is bonded in a 2-coordinate geometry to two Rb1+, one Ag+1.50+, and one P3+ atom.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-29. Materials Data on Rb2Ag2Sn(PSe3)3 by Materials Project. https://doi.org/10.17188/1750638

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↗