Search NASA⌕ Search

DOE OSTI · 1700762

Materials Data on Pr2S3O20 by Materials Project

Abstract

Pr2S3O20 crystallizes in the monoclinic Cc space group. The structure is two-dimensional and consists of two Pr2S3O20 sheets oriented in the (-1, 0, 1) direction. there are two inequivalent Pr sites. In the first Pr site, Pr is bonded in a 7-coordinate geometry to seven O atoms. There are a spread of Pr–O bond distances ranging from 2.39–2.68 Å. In the second Pr site, Pr is bonded in a 7-coordinate geometry to seven O atoms. There are a spread of Pr–O bond distances ranging from 2.30–3.11 Å. There are three inequivalent S sites. In the first S site, S is bonded in a tetrahedral geometry to four O atoms. There are a spread of S–O bond distances ranging from 1.43–1.86 Å. In the second S site, S is bonded in a tetrahedral geometry to four O atoms. There are a spread of S–O bond distances ranging from 1.48–1.50 Å. In the third S site, S is bonded in a tetrahedral geometry to four O atoms. There are a spread of S–O bond distances ranging from 1.47–1.51 Å. There are twenty inequivalent O sites. In the first O site, O is bonded in a distorted bent 150 degrees geometry to one Pr and one S atom. In the second O site, O is bonded in a single-bond geometry to one S atom. In the third O site, O is bonded in a bent 150 degrees geometry to one Pr and one S atom. In the fourth O site, O is bonded in a distorted linear geometry to one Pr and one S atom. In the fifth O site, O is bonded in a distorted bent 150 degrees geometry to one Pr and one S atom. In the sixth O site, O is bonded in a single-bond geometry to one S atom. In the seventh O site, O is bonded in a distorted bent 150 degrees geometry to one Pr and one S atom. In the eighth O site, O is bonded in a linear geometry to one Pr and one S atom. In the ninth O site, O is bonded in a single-bond geometry to one S atom. In the tenth O site, O is bonded in a 1-coordinate geometry to one Pr and one S atom. In the eleventh O site, O is bonded in a distorted bent 120 degrees geometry to one Pr and one S atom. In the twelfth O site, O is bonded in a bent 120 degrees geometry to one S and one O atom. The O–O bond length is 1.31 Å. In the thirteenth O site, O is bonded in a water-like geometry to one Pr and one O atom. The O–O bond length is 1.23 Å. In the fourteenth O site, O is bonded in a single-bond geometry to one O atom. In the fifteenth O site, O is bonded in a single-bond geometry to one Pr atom. In the sixteenth O site, O is bonded in a bent 120 degrees geometry to one Pr and one O atom. In the seventeenth O site, O is bonded in a distorted bent 120 degrees geometry to one Pr and one O atom. The O–O bond length is 1.23 Å. In the eighteenth O site, O is bonded in a single-bond geometry to one Pr atom. In the nineteenth O site, O is bonded in a single-bond geometry to one Pr atom. In the twentieth O site, O is bonded in a single-bond geometry to one O atom.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-29. Materials Data on Pr2S3O20 by Materials Project. https://doi.org/10.17188/1700762

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↗