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25 records · Page 2

Materials Data on C3S8 by Materials Project

C3S8 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of two [1,3]dithiolo[4,5-f]pentathiepine-7-thione molecules. there are three inequivalent C4+ sites. In the first C4+ site, C4+ is bonded in a distorted bent 120 degrees geometry to one C4+ and two S+1.50- atoms. The C–C bond length is 1.37 Å. There is one shorter (1.74 Å) and one longer (1.76 Å) C–S bond length. In the second C4+ site, C4+ is bonded in a distorted bent 120 degrees geometry to one C4+ and two S+1.50- atoms. There is one shorter (1.74 Å) and one longer (1.76 Å) C–S bond length. In the third C4+ site, C4+ is bonded in a trigonal planar geometry to three S+1.50- atoms. There is one shorter (1.65 Å) and two longer (1.75 Å) C–S bond length. There are eight inequivalent S+1.50- sites. In the first S+1.50- site, S+1.50- is bonded in a distorted water-like geometry to one C4+ and one S+1.50- atom. The S–S bond length is 2.07 Å. In the second S+1.50- site, S+1.50- is bonded in a distorted water-like geometry to two S+1.50- atoms. The S–S bond length is 2.07 Å. In the third S+1.50- site, S+1.50- is bonded in a water-like geometry to two S+1.50- atoms. The S–S bond length is 2.07 Å. In the fourth S+1.50- site, S+1.50- is bonded in a water-like geometry to two S+1.50- atoms. The S–S bond length is 2.07 Å. In the fifth S+1.50- site, S+1.50- is bonded in a distorted water-like geometry to one C4+ and one S+1.50- atom. In the sixth S+1.50- site, S+1.50- is bonded in a water-like geometry to two C4+ atoms. In the seventh S+1.50- site, S+1.50- is bonded in a water-like geometry to two C4+ atoms. In the eighth S+1.50- site, S+1.50- is bonded in a single-bond geometry to one C4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on CS3 by Materials Project

CS3 crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of sixteen carbonotrithioic acid molecules. C2- is bonded in a trigonal planar geometry to three S+0.67+ atoms. All C–S bond lengths are 1.67 Å. There are three inequivalent S+0.67+ sites. In the first S+0.67+ site, S+0.67+ is bonded in a single-bond geometry to one C2- atom. In the second S+0.67+ site, S+0.67+ is bonded in a single-bond geometry to one C2- atom. In the third S+0.67+ site, S+0.67+ is bonded in a single-bond geometry to one C2- atom.

36 MATERIALS SCIENCE↗

Materials Data on C3S4 by Materials Project

C3S4 crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of two 3h,7h-1,2,4,5,6,8-hexathia-s-indacene-3,7-dithione molecules and four C3S4 clusters. In each C3S4 cluster, there are three inequivalent C+2.67+ sites. In the first C+2.67+ site, C+2.67+ is bonded in a distorted bent 120 degrees geometry to two S2- atoms. There is one shorter (1.74 Å) and one longer (1.75 Å) C–S bond length. In the second C+2.67+ site, C+2.67+ is bonded in a distorted single-bond geometry to one S2- atom. The C–S bond length is 1.77 Å. In the third C+2.67+ site, C+2.67+ is bonded in a bent 120 degrees geometry to two S2- atoms. There is one shorter (1.67 Å) and one longer (1.73 Å) C–S bond length. There are four inequivalent S2- sites. In the first S2- site, S2- is bonded in a water-like geometry to two C+2.67+ atoms. In the second S2- site, S2- is bonded in a 2-coordinate geometry to one C+2.67+ and one S2- atom. The S–S bond length is 2.07 Å. In the third S2- site, S2- is bonded in a distorted water-like geometry to one C+2.67+ and one S2- atom. In the fourth S2- site, S2- is bonded in a single-bond geometry to one C+2.67+ atom.

36 MATERIALS SCIENCE↗

Materials Data on CS30 by Materials Project

S30C crystallizes in the monoclinic C2/m space group. The structure is zero-dimensional and consists of twelve hydrogen disulfide molecules, eight hydrogen sulfide molecules, two CS2 clusters, and eight S clusters. In each CS2 cluster, C4+ is bonded in a linear geometry to two equivalent S+0.13- atoms. Both C–S bond lengths are 1.55 Å. S+0.13- is bonded in a single-bond geometry to one C4+ atom. In each S cluster, there are three inequivalent S+0.13- sites. In the first S+0.13- site, S+0.13- is bonded in a single-bond geometry to two S+0.13- atoms. There are one shorter (1.90 Å) and one longer (3.69 Å) S–S bond lengths. In the second S+0.13- site, S+0.13- is bonded in a single-bond geometry to two S+0.13- atoms. The S–S bond length is 3.85 Å. In the third S+0.13- site, S+0.13- is bonded in a 1-coordinate geometry to two S+0.13- atoms.

36 MATERIALS SCIENCE↗

Materials Data on CS by Materials Project

SC1 is lead oxide structured and crystallizes in the tetragonal P4/nmm space group. The structure is two-dimensional and consists of one SC1 sheet oriented in the (0, 0, 1) direction. C2+ is bonded to four equivalent S2- atoms to form a mixture of distorted edge and corner-sharing CS4 trigonal pyramids. All C–S bond lengths are 1.90 Å. S2- is bonded in a distorted see-saw-like geometry to four equivalent C2+ atoms.

36 MATERIALS SCIENCE↗

MEMS-Based Micro Instruments for In-Situ Planetary Exploration

NASA's planetary exploration strategy is primarily targeted to the detection of extant or extinct signs of life. Thus, the agency is moving towards more in-situ landed missions as evidenced by the recent, successful demonstration of twin Mars Exploration Rovers. Also, future robotic exploration platforms are expected to evolve towards sophisticated analytical laboratories composed of multi-instrument suites. MEMS technology is very attractive for in-situ planetary exploration because of the promise of a diverse and capable set of advanced, low mass and low-power devices and instruments. At JPL, we are exploiting this diversity of MEMS for the development of a new class of miniaturized instruments for planetary exploration. In particular, two examples of this approach are the development of an Electron Luminescence X-ray Spectrometer (ELXS), and a Force-Detected Nuclear Magnetic Resonance (FDNMR) Spectrometer.

micro instruments↗

CFD Comparisons with Updated NASA Juncture Flow Data

The purpose of the NASA Juncture Flow experiment is to acquire high-quality flowfield details deep in the corner of a wing-body junction specifically for the purpose of CFD validation. A second phase of testing was recently completed, which includes both laser doppler velocimetry and particle image velocimetry measurements. This paper describes the recent experiment and its results. It also makes detailed comparisons between the experimental data and a new version of a widely-used CFD turbulence model for Reynolds-averaged Navier-Stokes, which was recently developed to improve separated corner flow predictions. The CFD results generally produce very good qualitative agreement with the experiment, although they are less accurate inside of the separation region, as expected.

Experimental Data↗