Engineering Papers⌕ Search

DOE OSTI · 1718151

Materials Data on Ba5P3O13 by Materials Project

Abstract

Ba5P3O13 crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. there are five inequivalent Ba sites. In the first Ba site, Ba is bonded in a 7-coordinate geometry to seven O atoms. There are a spread of Ba–O bond distances ranging from 2.70–2.96 Å. In the second Ba site, Ba is bonded in a 7-coordinate geometry to seven O atoms. There are a spread of Ba–O bond distances ranging from 2.69–2.96 Å. In the third Ba site, Ba is bonded in a 7-coordinate geometry to seven O atoms. There are a spread of Ba–O bond distances ranging from 2.67–2.98 Å. In the fourth Ba site, Ba is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of Ba–O bond distances ranging from 2.71–3.17 Å. In the fifth Ba site, Ba is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of Ba–O bond distances ranging from 2.77–3.04 Å. There are three inequivalent P sites. In the first P site, P is bonded in a tetrahedral geometry to four O atoms. All P–O bond lengths are 1.56 Å. In the second P site, P is bonded in a tetrahedral geometry to four O atoms. All P–O bond lengths are 1.56 Å. In the third P site, P is bonded in a tetrahedral geometry to four O atoms. All P–O bond lengths are 1.56 Å. There are thirteen inequivalent O sites. In the first O site, O is bonded in a distorted single-bond geometry to three Ba and one P atom. In the second O site, O is bonded in a distorted single-bond geometry to three Ba and one P atom. In the third O site, O is bonded in a distorted single-bond geometry to three Ba and one P atom. In the fourth O site, O is bonded in a distorted single-bond geometry to three Ba and one P atom. In the fifth O site, O is bonded in a distorted single-bond geometry to three Ba and one P atom. In the sixth O site, O is bonded in a distorted single-bond geometry to three Ba and one P atom. In the seventh O site, O is bonded in a distorted single-bond geometry to three Ba and one P atom. In the eighth O site, O is bonded in a distorted single-bond geometry to three Ba and one P atom. In the ninth O site, O is bonded in a distorted single-bond geometry to three Ba and one P atom. In the tenth O site, O is bonded in a distorted single-bond geometry to three Ba and one P atom. In the eleventh O site, O is bonded in a distorted single-bond geometry to three Ba and one P atom. In the twelfth O site, O is bonded in a distorted single-bond geometry to three Ba and one P atom. In the thirteenth O site, O is bonded in a trigonal non-coplanar geometry to three Ba atoms.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-04-30. Materials Data on Ba5P3O13 by Materials Project. https://doi.org/10.17188/1718151

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↗