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At least 37 records · Page 2

Materials Data on Dy(SiRu)2 by Materials Project

DyRu2Si2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Dy3+ is bonded in a 8-coordinate geometry to eight equivalent Si4- atoms. All Dy–Si bond lengths are 3.22 Å. Ru+2.50+ is bonded to four equivalent Si4- atoms to form a mixture of corner and edge-sharing RuSi4 tetrahedra. All Ru–Si bond lengths are 2.38 Å. Si4- is bonded in a 4-coordinate geometry to four equivalent Dy3+ and four equivalent Ru+2.50+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Pr(SiRu)2 by Materials Project

PrRu2Si2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Pr3+ is bonded in a distorted body-centered cubic geometry to eight equivalent Si4- atoms. All Pr–Si bond lengths are 3.28 Å. Ru+2.50+ is bonded to four equivalent Si4- atoms to form a mixture of corner and edge-sharing RuSi4 tetrahedra. All Ru–Si bond lengths are 2.39 Å. Si4- is bonded in a 4-coordinate geometry to four equivalent Pr3+ and four equivalent Ru+2.50+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Er(SiRu)2 by Materials Project

ErRu2Si2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Er3+ is bonded in a 8-coordinate geometry to eight equivalent Si4- atoms. All Er–Si bond lengths are 3.21 Å. Ru+2.50+ is bonded to four equivalent Si4- atoms to form a mixture of corner and edge-sharing RuSi4 tetrahedra. All Ru–Si bond lengths are 2.38 Å. Si4- is bonded in a 4-coordinate geometry to four equivalent Er3+ and four equivalent Ru+2.50+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on La(SiRu)2 by Materials Project

LaRu2Si2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. La3+ is bonded in a distorted body-centered cubic geometry to eight equivalent Si4- atoms. All La–Si bond lengths are 3.31 Å. Ru+2.50+ is bonded to four equivalent Si4- atoms to form a mixture of distorted edge and corner-sharing RuSi4 tetrahedra. All Ru–Si bond lengths are 2.40 Å. Si4- is bonded in a 4-coordinate geometry to four equivalent La3+ and four equivalent Ru+2.50+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Th(SiRu)2 by Materials Project

ThRu2Si2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Th4+ is bonded in a 8-coordinate geometry to eight equivalent Si4- atoms. All Th–Si bond lengths are 3.26 Å. Ru2+ is bonded to four equivalent Si4- atoms to form a mixture of edge and corner-sharing RuSi4 tetrahedra. All Ru–Si bond lengths are 2.41 Å. Si4- is bonded in a 4-coordinate geometry to four equivalent Th4+ and four equivalent Ru2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Ho(SiRu)2 by Materials Project

HoRu2Si2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Ho3+ is bonded in a 8-coordinate geometry to eight equivalent Si4- atoms. All Ho–Si bond lengths are 3.21 Å. Ru+2.50+ is bonded to four equivalent Si4- atoms to form a mixture of edge and corner-sharing RuSi4 tetrahedra. All Ru–Si bond lengths are 2.38 Å. Si4- is bonded in a 4-coordinate geometry to four equivalent Ho3+ and four equivalent Ru+2.50+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Tm(SiRu)2 by Materials Project

TmRu2Si2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Tm3+ is bonded in a 8-coordinate geometry to eight equivalent Si4- atoms. All Tm–Si bond lengths are 3.20 Å. Ru+2.50+ is bonded to four equivalent Si4- atoms to form a mixture of edge and corner-sharing RuSi4 tetrahedra. All Ru–Si bond lengths are 2.38 Å. Si4- is bonded in a 9-coordinate geometry to four equivalent Tm3+ and four equivalent Ru+2.50+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Y(SiRu)2 by Materials Project

YRu2Si2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Y3+ is bonded in a 8-coordinate geometry to eight equivalent Si4- atoms. All Y–Si bond lengths are 3.22 Å. Ru+2.50+ is bonded to four equivalent Si4- atoms to form a mixture of corner and edge-sharing RuSi4 tetrahedra. All Ru–Si bond lengths are 2.38 Å. Si4- is bonded in a 4-coordinate geometry to four equivalent Y3+ and four equivalent Ru+2.50+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Gd(SiRu)2 by Materials Project

GdRu2Si2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Gd3+ is bonded in a 8-coordinate geometry to eight equivalent Si4- atoms. All Gd–Si bond lengths are 3.23 Å. Ru+2.50+ is bonded to four equivalent Si4- atoms to form a mixture of corner and edge-sharing RuSi4 tetrahedra. All Ru–Si bond lengths are 2.39 Å. Si4- is bonded in a 4-coordinate geometry to four equivalent Gd3+ and four equivalent Ru+2.50+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Eu(SiRu)2 by Materials Project

EuRu2Si2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Eu2+ is bonded in a 8-coordinate geometry to eight equivalent Si4- atoms. All Eu–Si bond lengths are 3.30 Å. Ru3+ is bonded to four equivalent Si4- atoms to form a mixture of distorted edge and corner-sharing RuSi4 tetrahedra. All Ru–Si bond lengths are 2.39 Å. Si4- is bonded in a 4-coordinate geometry to four equivalent Eu2+ and four equivalent Ru3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on ZrNb(SiRu)2 by Materials Project

ZrNb(RuSi)2 crystallizes in the monoclinic Pm space group. The structure is three-dimensional. there are three inequivalent Zr2+ sites. In the first Zr2+ site, Zr2+ is bonded to five Si4- atoms to form ZrSi5 square pyramids that share corners with five ZrSi5 square pyramids, corners with five NbSi5 square pyramids, corners with six RuSi4 tetrahedra, edges with two NbSi5 square pyramids, edges with four ZrSi5 square pyramids, and edges with six RuSi4 tetrahedra. There are four shorter (2.74 Å) and one longer (2.77 Å) Zr–Si bond lengths. In the second Zr2+ site, Zr2+ is bonded to five Si4- atoms to form ZrSi5 square pyramids that share a cornercorner with one ZrSi5 square pyramid, corners with nine NbSi5 square pyramids, corners with six RuSi4 tetrahedra, edges with two equivalent ZrSi5 square pyramids, edges with four NbSi5 square pyramids, and edges with six RuSi4 tetrahedra. There are three shorter (2.75 Å) and two longer (2.77 Å) Zr–Si bond lengths. In the third Zr2+ site, Zr2+ is bonded to five Si4- atoms to form ZrSi5 square pyramids that share corners with four equivalent ZrSi5 square pyramids, corners with six NbSi5 square pyramids, corners with six RuSi4 tetrahedra, edges with two NbSi5 square pyramids, edges with four ZrSi5 square pyramids, and edges with six RuSi4 tetrahedra. There are a spread of Zr–Si bond distances ranging from 2.74–2.77 Å. There are three inequivalent Nb2+ sites. In the first Nb2+ site, Nb2+ is bonded to five Si4- atoms to form distorted NbSi5 square pyramids that share corners with three equivalent NbSi5 square pyramids, corners with seven ZrSi5 square pyramids, corners with six RuSi4 tetrahedra, edges with three ZrSi5 square pyramids, edges with three NbSi5 square pyramids, and edges with six RuSi4 tetrahedra. There are a spread of Nb–Si bond distances ranging from 2.68–2.76 Å. In the second Nb2+ site, Nb2+ is bonded to five Si4- atoms to form NbSi5 square pyramids that share corners with two equivalent NbSi5 square pyramids, corners with eight ZrSi5 square pyramids, corners with six RuSi4 tetrahedra, edges with three ZrSi5 square pyramids, edges with three NbSi5 square pyramids, and edges with six RuSi4 tetrahedra. There are a spread of Nb–Si bond distances ranging from 2.69–2.72 Å. In the third Nb2+ site, Nb2+ is bonded to five Si4- atoms to form NbSi5 square pyramids that share corners with five ZrSi5 square pyramids, corners with five NbSi5 square pyramids, corners with six RuSi4 tetrahedra, edges with two equivalent ZrSi5 square pyramids, edges with four NbSi5 square pyramids, and edges with six RuSi4 tetrahedra. There are two shorter (2.70 Å) and three longer (2.72 Å) Nb–Si bond lengths. There are six inequivalent Ru2+ sites. In the first Ru2+ site, Ru2+ is bonded to four Si4- atoms to form RuSi4 tetrahedra that share corners with two equivalent NbSi5 square pyramids, corners with four ZrSi5 square pyramids, corners with ten RuSi4 tetrahedra, edges with two equivalent ZrSi5 square pyramids, edges with four NbSi5 square pyramids, and edges with two RuSi4 tetrahedra. There are a spread of Ru–Si bond distances ranging from 2.48–2.51 Å. In the second Ru2+ site, Ru2+ is bonded to four Si4- atoms to form RuSi4 tetrahedra that share corners with two equivalent ZrSi5 square pyramids, corners with four NbSi5 square pyramids, corners with ten RuSi4 tetrahedra, edges with two equivalent NbSi5 square pyramids, edges with four ZrSi5 square pyramids, and edges with two RuSi4 tetrahedra. There are a spread of Ru–Si bond distances ranging from 2.51–2.54 Å. In the third Ru2+ site, Ru2+ is bonded to four Si4- atoms to form RuSi4 tetrahedra that share corners with two equivalent NbSi5 square pyramids, corners with four ZrSi5 square pyramids, corners with ten RuSi4 tetrahedra, edges with two equivalent ZrSi5 square pyramids, edges with four NbSi5 square pyramids, and edges with two RuSi4 tetrahedra. There are a spread of Ru–Si bond distances ranging from 2.46–2.52 Å. In the fourth Ru2+ site, Ru2+ is bonded to four Si4- atoms to form RuSi4 tetrahedra that share corners with two equivalent ZrSi5 square pyramids, corners with four NbSi5 square pyramids, corners with ten RuSi4 tetrahedra, edges with two equivalent NbSi5 square pyramids, edges with four ZrSi5 square pyramids, and edges with two RuSi4 tetrahedra. There are a spread of Ru–Si bond distances ranging from 2.48–2.57 Å. In the fifth Ru2+ site, Ru2+ is bonded to four Si4- atoms to form RuSi4 tetrahedra that share corners with two equivalent ZrSi5 square pyramids, corners with four NbSi5 square pyramids, corners with ten RuSi4 tetrahedra, edges with two equivalent ZrSi5 square pyramids, edges with four NbSi5 square pyramids, and edges with two RuSi4 tetrahedra. There are a spread of Ru–Si bond distances ranging from 2.44–2.57 Å. In the sixth Ru2+ site, Ru2+ is bonded to four Si4- atoms to form RuSi4 tetrahedra that share corners with two equivalent NbSi5 square pyramids, corners with four ZrSi5 square pyramids, corners with ten RuSi4 tetrahedra, edges with two equivalent NbSi5 square pyramids, edges with four ZrSi5 square pyramids, and edges with two RuSi4 tetrahedra. There are a spread of Ru–Si bond distances ranging from 2.45–2.58 Å. There are six inequivalent Si4- sites. In the first Si4- site, Si4- is bonded in a 9-coordinate geometry to two equivalent Zr2+, four Nb2+, and three Ru2+ atoms. In the second Si4- site, Si4- is bonded in a 9-coordinate geometry to four Zr2+, two equivalent Nb2+, and three Ru2+ atoms. In the third Si4- site, Si4- is bonded in a 9-coordinate geometry to two equivalent Zr2+, four Nb2+, and three Ru2+ atoms. In the fourth Si4- site, Si4- is bonded in a 9-coordinate geometry to four Zr2+, two equivalent Nb2+, and three Ru2+ atoms. In the fifth Si4- site, Si4- is bonded in a 9-coordinate geometry to one Zr2+, two Nb2+, and six Ru2+ atoms. In the sixth Si4- site, Si4- is bonded in a 9-coordinate geometry to two Zr2+, one Nb2+, and six Ru2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Sm3(SiRu)2 by Materials Project

Sm3Ru2Si2 crystallizes in the orthorhombic Pbcm space group. The structure is three-dimensional. there are two inequivalent Sm sites. In the first Sm site, Sm is bonded in a 9-coordinate geometry to four equivalent Ru and five Si atoms. There are two shorter (3.06 Å) and two longer (3.19 Å) Sm–Ru bond lengths. There are a spread of Sm–Si bond distances ranging from 2.99–3.36 Å. In the second Sm site, Sm is bonded in a 6-coordinate geometry to four equivalent Ru and five Si atoms. There are a spread of Sm–Ru bond distances ranging from 2.86–3.09 Å. There are a spread of Sm–Si bond distances ranging from 3.06–3.55 Å. Ru is bonded in a 9-coordinate geometry to six Sm and three Si atoms. There are a spread of Ru–Si bond distances ranging from 2.50–2.54 Å. There are two inequivalent Si sites. In the first Si site, Si is bonded in a 9-coordinate geometry to seven Sm and two equivalent Ru atoms. In the second Si site, Si is bonded in a 12-coordinate geometry to eight Sm and four equivalent Ru atoms.

36 MATERIALS SCIENCE↗

Materials Data on ZrTa(SiRu)2 by Materials Project

ZrTa(RuSi)2 crystallizes in the monoclinic Pm space group. The structure is three-dimensional. there are three inequivalent Zr sites. In the first Zr site, Zr is bonded in a 11-coordinate geometry to six Ru and five Si atoms. There are a spread of Zr–Ru bond distances ranging from 2.89–3.07 Å. There are four shorter (2.74 Å) and one longer (2.78 Å) Zr–Si bond lengths. In the second Zr site, Zr is bonded in a 11-coordinate geometry to six Ru and five Si atoms. There are a spread of Zr–Ru bond distances ranging from 2.87–3.06 Å. There are a spread of Zr–Si bond distances ranging from 2.74–2.76 Å. In the third Zr site, Zr is bonded in a 11-coordinate geometry to six Ru and five Si atoms. There are a spread of Zr–Ru bond distances ranging from 2.90–3.06 Å. There are four shorter (2.74 Å) and one longer (2.79 Å) Zr–Si bond lengths. There are three inequivalent Ta sites. In the first Ta site, Ta is bonded in a 11-coordinate geometry to six Ru and five Si atoms. There are a spread of Ta–Ru bond distances ranging from 2.87–3.06 Å. There are a spread of Ta–Si bond distances ranging from 2.68–2.74 Å. In the second Ta site, Ta is bonded in a 11-coordinate geometry to six Ru and five Si atoms. There are a spread of Ta–Ru bond distances ranging from 2.88–3.06 Å. There are four shorter (2.69 Å) and one longer (2.71 Å) Ta–Si bond lengths. In the third Ta site, Ta is bonded in a 11-coordinate geometry to six Ru and five Si atoms. There are a spread of Ta–Ru bond distances ranging from 2.88–3.05 Å. There are a spread of Ta–Si bond distances ranging from 2.70–2.72 Å. There are six inequivalent Ru sites. In the first Ru site, Ru is bonded in a 12-coordinate geometry to four Zr, two equivalent Ta, two Ru, and four Si atoms. There are one shorter (2.80 Å) and one longer (2.82 Å) Ru–Ru bond lengths. There are two shorter (2.51 Å) and two longer (2.52 Å) Ru–Si bond lengths. In the second Ru site, Ru is bonded in a 12-coordinate geometry to two equivalent Zr, four Ta, two Ru, and four Si atoms. There are one shorter (2.77 Å) and one longer (2.81 Å) Ru–Ru bond lengths. There are a spread of Ru–Si bond distances ranging from 2.46–2.51 Å. In the third Ru site, Ru is bonded in a 12-coordinate geometry to two equivalent Zr, four Ta, two Ru, and four Si atoms. The Ru–Ru bond length is 2.77 Å. There are three shorter (2.47 Å) and one longer (2.50 Å) Ru–Si bond lengths. In the fourth Ru site, Ru is bonded in a 12-coordinate geometry to four Zr, two equivalent Ta, two Ru, and four Si atoms. The Ru–Ru bond length is 2.76 Å. There are a spread of Ru–Si bond distances ranging from 2.48–2.57 Å. In the fifth Ru site, Ru is bonded in a 12-coordinate geometry to two equivalent Zr, four Ta, two Ru, and four Si atoms. There are a spread of Ru–Si bond distances ranging from 2.44–2.54 Å. In the sixth Ru site, Ru is bonded in a 12-coordinate geometry to four Zr, two equivalent Ta, two Ru, and four Si atoms. There are a spread of Ru–Si bond distances ranging from 2.45–2.58 Å. There are six inequivalent Si sites. In the first Si site, Si is bonded in a 9-coordinate geometry to one Zr, two Ta, and six Ru atoms. In the second Si site, Si is bonded in a 9-coordinate geometry to two Zr, one Ta, and six Ru atoms. In the third Si site, Si is bonded in a 9-coordinate geometry to two equivalent Zr, four Ta, and three Ru atoms. In the fourth Si site, Si is bonded in a 9-coordinate geometry to four Zr, two equivalent Ta, and three Ru atoms. In the fifth Si site, Si is bonded in a 9-coordinate geometry to two equivalent Zr, four Ta, and three Ru atoms. In the sixth Si site, Si is bonded in a 9-coordinate geometry to four Zr, two equivalent Ta, and three Ru atoms.

36 MATERIALS SCIENCE↗

SIRU development. Volume 2: Gyro module

The design, operation, performance and test of the gyro module and its circuit components are described for the Strapdown Inertial Reverence Unit system.

Cooper, R.↗

Determination of the dispersion constant in a constrained vapor bubble thermosyphon

The isothermal profiles of the extended meniscus in a quartz cuvette were measured in a gravitational field using an image analyzing interferometer which is based on computer enhanced video microscopy of the naturally occurring interference fringes. The experimental results for heptane and pentane menisci were analyzed using the extended Young Laplace Equation. These isothermal results characterized the interfacial force field in-siru at the start of the heat transfer experiments by quantifying the dispersion constant, which is a function of the liquid-solid system and cleaning procedures. The experimentally obtained values of the disjoining pressure and the dispersion constants were compared to that predicted from the DLP theory and good agreements were obtained. The measurements are critical to the subsequent non-isothermal experiments because one of the major variables in the heat sink capability of the Constrained Vapor Bubble Thermosyphon, CVBT, is the dispersion constant. In all previous studies of micro heat pipes the value of the dispersion constant has been 'estimated'. One of the major advantages of the current glass cell is the ability to view the extended meniscus at all times. Experimentally, we find that the extended Young-Laplace Equation is an excellent model for the force field at the solid-liquid-vapor interfaces.

Dasgupta, Sunando↗