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Online since: March 2026
Authors: Nur Ain Atisya C.M. Khairuddin, Mohd Hasmizam Razali, Alina Irwana Muhamad A'srai
When coupled with WO3, transition metal dichalcogenides such as tungsten disulfide (WS2) can improve charge separation and surface area by providing layered structures and exceptional electrical conductivity, resulting in effective heterostructures [4].
Results and Discussion The XRD patterns of WO3/WS2 composites loaded with different metal nanoparticles specifically (a) Au, (b) Ag, (c) Ru, (d) Rh, and (e) Pt were confirm the successful formation of multi-phase crystalline structures in Fig. 1.
In sample (a), the Au@ WO3/WS2 composite exhibits extra peaks at 19.1° (111), which correspond to the gold nanoparticles' face-centered cubic (fcc) structure (JCPDS 04-0784).
The Au@WO3/WS2 composite exhibits a tight, layered structure with minimal porosity and particle agglomeration.
Journal of Materials Chemistry A, 6(10), 4271–4292. https://doi.org/10.1039/C7TA09335G
Online since: October 2010
Authors: Hong Wei Xie, Jin Xia Wang, Yu Chun Zhai, Cheng De Li, Xiao Yun Hu
The structure and transport mechanisms of the melt can be known by the electrical conductivity, and the power consumption can also be calculated used it.
The density plays important role in the separation of liquid phases, and can reflected the structure of the electrolytes indirectly.
Secondly the crystal of sodium chloride is typically ionic structure, however that of calcium chloride is a transition structure between ionic structure and molecular structure.
Wang, Researching methods on physical chemistry of metallurgy( Metallurgical Industry Press, Chinese1981)
Online since: June 2014
Authors: Fei Chen, Qiang Shen, Lian Meng Zhang, Rong Tu, Yan Hua Zhang
In order to find an improved synthesis process, it is important to know how Al affects the structure and conductivity in the LLZO solid electrolyte.
Akimoto, Crystal structure of fast lithium-ion-conducting cubic Li7La3Zr2O12, Chem.
Goodenough, Low-temperature synthesis of Li7La3Zr2O12 with cubic garnet-type structure, Mater.
Weppner, Crystal chemistry and stability of “Li7La3Zr2O12” garnet: a fast lithium-ion conductor, Inorg.
Stefan, Structure and dynamics of the fast lithium ion conductor "Li7La3Zr2O12", Phys.
Online since: September 2020
Authors: Giovanna Brunetti, Antonino Rizzuti, Piero Mastrorilli, Michele Dassisti
This is due to the particles forming chain-like structures (MR structures) parallel to the magnetic field lines.
In the on-state, instead, nanoparticles fill the voids between micron-sized particles regularizing MR structures.
HARD and SOFT particles differ from each other for their skin structure, mechanical properties, Fe and other elements content.
In this process, producing mechanically soft particles, the onion skin structure is lost, and the content of C, N and O is reduced.
Wereley (Ed.), RSC Smart Materials, Royal Society of Chemistry, Cambridge 2013, pp 31–55
Online since: July 2019
Authors: Xiao Wu Li, Dong Han, Le Le Kang
The dislocation structures of all Cu-5at.
%Mn alloys are fully featured by dislocation cells, which are the typical wavy-slip type dislocation structure [19].
%Mn alloys with different t, planar-slip dislocation structures are the common plastic deformation micro-features, as shown in Fig. 6.
It is worth noticing that, compared with wavy-slip dislocation structures, planar slip structures can suppress the annihilation of dislocations and assist the strain-hardening process by reducing the dislocation glide length, leading to the enhancement in plastic defomation capacity [17-19].
Wang, Plastic-strain-amplitude dependence of dislocation structures in cyclically deformed <112>-oriented Cu-7 at. pct Al alloy single crystals, Metall.
Online since: May 2014
Authors: Gerardo Antonio Rosas Trejo, J. Luis López-Miranda, M.A. Espinosa-Medina, Rodrigo Alonso Esparza Muñoz, J.R. Romero-Romero
The bayerite phase has a monoclinic structure (ICSD #26830) and lattice parameters of a=5.062 Å, b=8.671 Å, c=4.713 Å, (β=90.27°).
The lattice fringes from the image were used in determining the d-spacing of the crystal structure of the powders.
Liu, Recent advances in ordered intermetallics, Materials Chemistry and Physics 42 (1995) 77-86
Black, The structure of FeAI2 by anomalous dispersion methods, Acta Cryst.
Black, The structure of FeA13 II, Acta Cryst. 8 (1955) 175
Online since: September 2013
Authors: Jian Feng Mo, Fei Jiao, Gong Li Zhang, Hui Yang, Shi Ping Pan
” (2)The characteristics of the food machinery 1) A wide variety of more complex operation principle, structure forms, and may vary from.
Knowledge involved in the production of food machinery is very broad and includes not only the content of the general machinery, but also to food engineering, food chemistry, food rheology, food hygiene and plastic arts.
The typical structure of box-type, its structure is simple.
In order to achieve the whole structure is simple, compact, easy to maintain, low cost requirements.
Instantaneous transmission ratio constant, the transmission efficiency can be as high as 98% to 99%, reliable, long life, compact structure, scope, from less than 1 kW to tens of thousands of kW.
Online since: March 2017
Authors: Alina Elena Toma
The groups fluoro-carbon and carbon-carbon form the strongest known organic links in chemistry.
Action on structures.
Design of steel structures.
Design of steel structures.
Design of aluminium structures.
Online since: November 2007
Authors: Ian William Murray Brown, Kenneth MacKenzie, M.E. Bowden, A. Kirchner, T. Kemmitt
These materials are X-ray amorphous and develop crystalline structure on extended heating at elevated temperature.
The TG-DSC curves for these two X-ray amorphous materials (shown in Fig. 2) are clearly distinct and indicate substantive differences in their materials chemistry, as reflected in their differing chemical and physical responses to heat treatment.
The relic pore structure is clearly visible.
There are substantial differences apparent in the chemical structures of these materials that controls both their thermal processing and physical appearance.
XRD traces for the heated materials are reproduced elsewhere [1,2] but both data sets display a room temperature amorphous structure that is stable until the first DSC exotherm at over 800 °C, at which point a progressive sequence of transition alumina structures is generated.
Online since: October 2014
Authors: Vladimir Sokolovsky, Sergey Dub, Tetiana Prikhna, Viktor Moshchil, Michael Eisterer, Harald W. Weber, Xavier Chaud, Valeriy Kovylaev, Artem Kozyrev, Tetyana Basyuk, Vladimir Sverdun, Tatiana Serbenyuk, Nina Sergienko, Myroslav Karpets, Wolfgang Gawalek
Besides in the MgB2 structure there are usually inclusions of higher magnesium borides MgBx (x=4÷25) which can also act as pinning centers [4, 6, 7].
Figure 1c shows the structure of the material prepared with Ti at 1050 oC, 2 GPa, 1 h and that the Ti-containing inclusions (the most bright) are rather big to be pinning centers by themselves and rather randomly distributed in MgB2 structure.
Figure 2 shows structure and x-ray patterns of the materials with and without Ti additions prepared at 800 and 1050 oC at 2 GPa.
The possible explanation of this difference lies in a specific structure of the MgB2 samples in which the non-superconducting and superconducting regions were formed.
Mathemetics, Physics and Chemistry, 200 (2005) 81-90