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Online since: August 2012
Authors: Roman Przeliorz, Jaroslaw Piątkowski
Thermodynamic calculations were performed using a HSC Chemistry Ver 4.1 computer programme [11].
Scale morphology Studies of scale morphology aimed mainly at the determination what effect the temperature and corrosive environment might have on its structure and porosity.
Grosjean: Effect of alloying elements on the ignition resistance of magnesium alloys, Scripta Mater. 49 (2003), p. 225 [11] HSC Chemistry Ver 4,1, computer programme Finland, (1998) [12] J.F.
Scale morphology Studies of scale morphology aimed mainly at the determination what effect the temperature and corrosive environment might have on its structure and porosity.
Grosjean: Effect of alloying elements on the ignition resistance of magnesium alloys, Scripta Mater. 49 (2003), p. 225 [11] HSC Chemistry Ver 4,1, computer programme Finland, (1998) [12] J.F.
Online since: August 2004
Authors: Klaus Fritscher, Christoph Leyens, Uwe Schulz, R. Wirth, W. Braue
The
TGO formation process is a complex function of chemistry of both, the bond coat and the TBC
system as well as the heat treatment conditions and oxygen partial pressures employed [1, 2].
While the dark contrasted TGO sections primarily represent alumina-rich Al-Y-Oss compositions a composite grain protruding into the bond coat surface shows a significant Z-contrast change due to different yttrium concentrations in the core and shell structures respectively.
Yang: in High Temperature Corrosion Materials Chemistry III, eds.
While the dark contrasted TGO sections primarily represent alumina-rich Al-Y-Oss compositions a composite grain protruding into the bond coat surface shows a significant Z-contrast change due to different yttrium concentrations in the core and shell structures respectively.
Yang: in High Temperature Corrosion Materials Chemistry III, eds.
Online since: November 2010
Authors: Shao Jiang Lin, Da Peng Feng, Qi Nian Shi
Introduction
Austenitic stainless steels are widely used as structural materials and functional materials in modern industries such as chemistry, aerospace, auto-mobile, food production and medical fields for its good corrosion resistance and processing properties [1-3].
It could be seen that the part has a flat surface, and the sintered metallic structure looks dense and uniform.
A higher sintering temperature resulted in higher densification, smoother pore structure and smaller pore size.
This diffusion is useful in controlling the densification process during sintering, therefore, a denser structure is achieved at higher sintering temperature [17].
It is seen that, at higher sintering temperatures, a denser structure is formed due to higher diffusion rates [17].
It could be seen that the part has a flat surface, and the sintered metallic structure looks dense and uniform.
A higher sintering temperature resulted in higher densification, smoother pore structure and smaller pore size.
This diffusion is useful in controlling the densification process during sintering, therefore, a denser structure is achieved at higher sintering temperature [17].
It is seen that, at higher sintering temperatures, a denser structure is formed due to higher diffusion rates [17].
Online since: February 2013
Authors: Aissa Boudjella
Simulation Results
The MAS in (1D) dimension structure contains up to six DTB molecular units packed in the parallel geometrical arrangement.
With Ef close to LUMO, the conductance gap and VIP (the voltage interval between two peaks of to the same molecular structure (Fig. 3b)) are found to decrease, while the peak of the conductance increases.
The magnitude of the Fermi level position for each molecular structure (N=1,2, 3, 4 and 6), is indicated in Fig. 2, curves (Efo).
The magnitude of the Fermi level position for each molecular structure (N=1,2, 3, 4 and 6), is indicated in Fig. 2, curve (Efo+3d).
Cramer: Essential of computational chemistry: theories (Oxford University Press, U.S.A, 1994)
With Ef close to LUMO, the conductance gap and VIP (the voltage interval between two peaks of to the same molecular structure (Fig. 3b)) are found to decrease, while the peak of the conductance increases.
The magnitude of the Fermi level position for each molecular structure (N=1,2, 3, 4 and 6), is indicated in Fig. 2, curves (Efo).
The magnitude of the Fermi level position for each molecular structure (N=1,2, 3, 4 and 6), is indicated in Fig. 2, curve (Efo+3d).
Cramer: Essential of computational chemistry: theories (Oxford University Press, U.S.A, 1994)
Online since: September 2013
Authors: Naratip Vittayakorn, Wanwilai C. Vittayakorn, Dondanai Banjong
The potentiality of PTC barium titanate ceramic is demonstrated not only by the number of applications but also by the expertise acquired on structure-properties relationships in this material [5].
The crystal phase of BaTiO3 was tetragonal structure matched exactly with JCPDS file no. 76-0744.
Literatures reveal that in order to get high dielectric constant, the crystal structure should have high tetragonality [7].
Varela, Size Effect on Structure and Dielectric Properties of Nb-doped Barium Titanate, J.
Newnham, Structure-Property Relationships in Sensors, Crystallo.
The crystal phase of BaTiO3 was tetragonal structure matched exactly with JCPDS file no. 76-0744.
Literatures reveal that in order to get high dielectric constant, the crystal structure should have high tetragonality [7].
Varela, Size Effect on Structure and Dielectric Properties of Nb-doped Barium Titanate, J.
Newnham, Structure-Property Relationships in Sensors, Crystallo.
Online since: April 2013
Authors: Gerardo Antonio Rosas Trejo, E. García de León M., O. Téllez-Vázquez, C. Patiño-Carachure
However, the milled samples show the presence of B2 intermetallic structure and also XRD-reflections of α-phase which is an aluminum hydroxide (Al(OH)3).
The α-phase has a hexagonal structure and is well known in mineralogy as bayerite.
On the other hand, the intermetallic bcc structure and the atomic relationship used in the present study (Fe40Al60) could favor the hydrogen embrittlement reaction [15].
The atomic packaging as consequence of bigger interatomic distances is smaller than in the fcc structure, allowing the hydrogen to diffuse more easily through the lattice’s interstices and the structural defects.
Therefore, aluminum centered in bcc cells, react more easily with water, unlike when pure aluminum has typical structure fcc.
The α-phase has a hexagonal structure and is well known in mineralogy as bayerite.
On the other hand, the intermetallic bcc structure and the atomic relationship used in the present study (Fe40Al60) could favor the hydrogen embrittlement reaction [15].
The atomic packaging as consequence of bigger interatomic distances is smaller than in the fcc structure, allowing the hydrogen to diffuse more easily through the lattice’s interstices and the structural defects.
Therefore, aluminum centered in bcc cells, react more easily with water, unlike when pure aluminum has typical structure fcc.
Online since: January 2007
Authors: Sang Jin Lee, S.Y. Chun, P.W. Shin, J.W. Kim
As well, porous structure of
the synthesized powders are introduced.
The porous structure was due to the development of foams in the thick solution during the stirring and drying process.
The crystallized powder also showed porous structure.
The SEM micrograph of the crystalline YAG revealed soft and porous powder structure.
Wenk: Better Ceramics Through Chemistry I, (Materials Research Society, Pittsburgh, PA, 1984)
The porous structure was due to the development of foams in the thick solution during the stirring and drying process.
The crystallized powder also showed porous structure.
The SEM micrograph of the crystalline YAG revealed soft and porous powder structure.
Wenk: Better Ceramics Through Chemistry I, (Materials Research Society, Pittsburgh, PA, 1984)
Online since: January 2009
Authors: Yong Li Yang, Song Lin Lai, Shu Ying Cheng
Ministry of Education Key Laboratory of Analysis and Detection Technology for Food Safety, and
Department of Chemistry, Fuzhou University, Fuzhou, Fujian, 350108, China
2.
The structure of the thin films was characterized by a Philips X ,Pert-MPD X-ray diffraction spectroscopy(XRD)and a Philips XL30E Scanning Electron Microscope (SEM).
The XRD spectra indicates that the structure of the SnS:Ag films are strongly influenced by the doping concentration.
It indicates that all the films show an orthorhombic crystal structure.
The four images of the SnS films seem to be similar which exhibit granular surface structures.
The structure of the thin films was characterized by a Philips X ,Pert-MPD X-ray diffraction spectroscopy(XRD)and a Philips XL30E Scanning Electron Microscope (SEM).
The XRD spectra indicates that the structure of the SnS:Ag films are strongly influenced by the doping concentration.
It indicates that all the films show an orthorhombic crystal structure.
The four images of the SnS films seem to be similar which exhibit granular surface structures.
Online since: August 2013
Authors: Oldrich Zmeskal, Jan Pospisil, Jakub Altsmid, Stanislav Nespurek
Chemical structures of both materials are shown in Scheme 1.
These diagrams can be used for the determination of model electric circuits of the studied structures.
Fig. 3 Frequency dependences of admittance (Y, left) and phase shift (φ, right) of ITO/ZnPcSu-PCBM/Al structures.
Scheme 2 Equivalent circuit of the structure ZnPcSu-PCBM/Al.
Fig. 4 Cole-Cole diagrams of ITO/ZnPcSu-PCBM/Al structures.
These diagrams can be used for the determination of model electric circuits of the studied structures.
Fig. 3 Frequency dependences of admittance (Y, left) and phase shift (φ, right) of ITO/ZnPcSu-PCBM/Al structures.
Scheme 2 Equivalent circuit of the structure ZnPcSu-PCBM/Al.
Fig. 4 Cole-Cole diagrams of ITO/ZnPcSu-PCBM/Al structures.
Online since: February 2022
Authors: Ahmed Abd El-Moneim, Mohsen Ghali, Asma Ebrahim
The X-ray source is Cu Kα target generated at 30 kV and 30 mA with scan speed 5°/min. the powder morphology and structure were determined using scanning electron microscopy (SEM) and transmission electron microscopy (TEM).
The obtained PXRD, Fig.1 (b), shows the same structure with a high degree of agreement with previously reported data for MOF-801.
Fig. 2 (a) shows the sheet like structure of the prepared Ppy using FeCl3 as an oxidizing agent in presence of SDS as a dopant.
Structure evaluation of bismuth telluride (Bi2Te3) nanoparticles with enhanced Seebeck coefficient and low thermal conductivity.
Materials Chemistry Frontiers, 1(2), pp.380-386
The obtained PXRD, Fig.1 (b), shows the same structure with a high degree of agreement with previously reported data for MOF-801.
Fig. 2 (a) shows the sheet like structure of the prepared Ppy using FeCl3 as an oxidizing agent in presence of SDS as a dopant.
Structure evaluation of bismuth telluride (Bi2Te3) nanoparticles with enhanced Seebeck coefficient and low thermal conductivity.
Materials Chemistry Frontiers, 1(2), pp.380-386