Search NASA⌕ Search
Home/Archive/DOE OSTI

DOE OSTI · 1747162

Materials Data on PH9PtC3Cl2 by Materials Project

View original source ↗Read source document ↗Export metadata ↓

Abstract

PtC3PH9Cl2 crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of two PtC3PH9Cl2 clusters. Pt2- is bonded in a rectangular see-saw-like geometry to one P5+ and three Cl1- atoms. The Pt–P bond length is 2.22 Å. There are a spread of Pt–Cl bond distances ranging from 2.31–2.46 Å. There are three inequivalent C+3.33- sites. In the first C+3.33- site, C+3.33- is bonded to one P5+ and three H1+ atoms to form distorted corner-sharing CPH3 tetrahedra. The C–P bond length is 1.81 Å. There is one shorter (1.09 Å) and two longer (1.10 Å) C–H bond length. In the second C+3.33- site, C+3.33- is bonded to one P5+ and three H1+ atoms to form distorted corner-sharing CPH3 tetrahedra. The C–P bond length is 1.81 Å. All C–H bond lengths are 1.10 Å. In the third C+3.33- site, C+3.33- is bonded to one P5+ and three H1+ atoms to form distorted corner-sharing CPH3 tetrahedra. The C–P bond length is 1.82 Å. There is one shorter (1.09 Å) and two longer (1.10 Å) C–H bond length. P5+ is bonded in a distorted tetrahedral geometry to one Pt2- and three C+3.33- atoms. There are nine inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one C+3.33- atom. In the second H1+ site, H1+ is bonded in a single-bond geometry to one C+3.33- atom. In the third H1+ site, H1+ is bonded in a single-bond geometry to one C+3.33- atom. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to one C+3.33- atom. In the fifth H1+ site, H1+ is bonded in a single-bond geometry to one C+3.33- atom. In the sixth H1+ site, H1+ is bonded in a single-bond geometry to one C+3.33- atom. In the seventh H1+ site, H1+ is bonded in a single-bond geometry to one C+3.33- atom. In the eighth H1+ site, H1+ is bonded in a single-bond geometry to one C+3.33- atom. In the ninth H1+ site, H1+ is bonded in a single-bond geometry to one C+3.33- atom. There are two inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a single-bond geometry to one Pt2- atom. In the second Cl1- site, Cl1- is bonded in a water-like geometry to two equivalent Pt2- atoms.

Explore related subjects

36 MATERIALS SCIENCEC-Cl-H-P-Ptcrystal structurePH9PtC3Cl2

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

2020-05-01. Materials Data on PH9PtC3Cl2 by Materials Project. https://doi.org/10.17188/1747162

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related reports

DOE OSTI2026

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↗