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Online since: September 2014
Authors: P.T. A. Santos, C.M. Furtado, Polyana T.A. Santos, A.C.F.M. Costa
Both spectra show three bands below 1000 cm-1 attributed to the vibrations that are intrinsic to the (Al-O) tetrahedral sites and (Zn-O) octahedral of the spinel characteristic.
El-Sayed et al. (2002) (14);, when studied the influence of zinc in some properties of Ni-Zn ferrite obtained by the conventional solid oxide absorption bands observed below 1000 cm-1.
The results of this study confirm the results obtained by El-Sayed et al. (2002) [13].
United States Patent Application Publication, US 2003/0180780 Al, (2003)
El-Sayed: Ceram.
El-Sayed et al. (2002) (14);, when studied the influence of zinc in some properties of Ni-Zn ferrite obtained by the conventional solid oxide absorption bands observed below 1000 cm-1.
The results of this study confirm the results obtained by El-Sayed et al. (2002) [13].
United States Patent Application Publication, US 2003/0180780 Al, (2003)
El-Sayed: Ceram.
Online since: February 2013
Authors: Jing Feng Chen, Le Yang Dai, Shao Fen Lin, Wen Chun Wang
The solid state reaction process between elemental W and C powders during ball milling had been studied in detail by El-Eskandarany et al. [9].
Yamada et al. [15] has made a similar study.
El-Eskandarany et al. [20] ball milled the mixture of WO3+C+3Mg for 12 h, they found that most of the WO3 was reduced to W with a small amount of residual WC.
Sherif El-Eskandarany, A.A.
Sherif El-Eskandarany, M.
Yamada et al. [15] has made a similar study.
El-Eskandarany et al. [20] ball milled the mixture of WO3+C+3Mg for 12 h, they found that most of the WO3 was reduced to W with a small amount of residual WC.
Sherif El-Eskandarany, A.A.
Sherif El-Eskandarany, M.
Online since: March 2016
Authors: M.R. Sahar, Nurulhuda Mohammad Yusoff
Many researchers have found that the addition of nanoparticles could enhanced the optical and luminescence characteristics as has been reported by Amjad et al., (2014) [9] and Dousti et al., (2013) [10].
El-Mallawany,Tellurite Glasses Handbook, Physical Properties and Data, CRC Press, Boca Roton, FL, 2001
El-Diasty, A.
El-Mongy, Central Glass and Ceramic Research Institute Bulletin,32 (3) (1985) 53-56
El-Diasty, Current Opinion in Solid State and Materials Science.10 (2006) 217-229
El-Mallawany,Tellurite Glasses Handbook, Physical Properties and Data, CRC Press, Boca Roton, FL, 2001
El-Diasty, A.
El-Mongy, Central Glass and Ceramic Research Institute Bulletin,32 (3) (1985) 53-56
El-Diasty, Current Opinion in Solid State and Materials Science.10 (2006) 217-229
Online since: December 2012
Authors: Huai Ping Tang, Shao Wei Tong
The Benchmark II model was selected as the model for simulating, and the N-S component of the 1940 El wave was selected as the input load.
Iterative learning control can be traced back to 1978, in which year Uchiyama[5]presented the initial explicit formulation of ILC in Japanese, and Arimoto[6] et al. first introduced this control method in English, in 1984.
Youqing Wang[7] et al. studied and compared three kinds of control methods including ILC,RC and R2R, then the authors pointed out that ILC was a hot filed.
Smolders[8] et al. proposed a nonlinear iterative learning approach based on model.
The Benchmark II model was selected as the model for simulating, and the N-S component of the 1940 El wave was selected as the input load.
Iterative learning control can be traced back to 1978, in which year Uchiyama[5]presented the initial explicit formulation of ILC in Japanese, and Arimoto[6] et al. first introduced this control method in English, in 1984.
Youqing Wang[7] et al. studied and compared three kinds of control methods including ILC,RC and R2R, then the authors pointed out that ILC was a hot filed.
Smolders[8] et al. proposed a nonlinear iterative learning approach based on model.
The Benchmark II model was selected as the model for simulating, and the N-S component of the 1940 El wave was selected as the input load.
Online since: June 2012
Authors: Ai Guo Zhou, Tai Chao Su, Shang Sheng Li, Liang Li
Jaworska et al made the first attempt on this [10, 11].
Morgiel, et al, Ti3SiC2 as a bonding phase in diamond composites, J.
El-Raghy, Synthesis and characterization of a remarkable ceramic: Ti3SiC2, J.
Zhang, et al, Rapid synthesis of dense Ti3SiC2 by spark plasma sintering, J.
[23] El-Raghy T and Barsoum MW, Processing and mechanical properties of Ti3SiC2: part I: reaction path and microstructure evolution, J.
Morgiel, et al, Ti3SiC2 as a bonding phase in diamond composites, J.
El-Raghy, Synthesis and characterization of a remarkable ceramic: Ti3SiC2, J.
Zhang, et al, Rapid synthesis of dense Ti3SiC2 by spark plasma sintering, J.
[23] El-Raghy T and Barsoum MW, Processing and mechanical properties of Ti3SiC2: part I: reaction path and microstructure evolution, J.
Online since: January 2015
Authors: Ivan R. Fateev, Artem V. Vukolov, Leonid G. Sukhikh, Sergey R. Uglov
Curve 4 shows the photon transmittance through a 1 μm thick Al foil.
Curves 1a, 2a, 3a and 4a show angular distributions of BTR taking absorption in the Al filter into account and are multiplied by factor of 5.
Curves 1a, 2a, 3a and 4a in Fig. 5 show the angular distributions of the BTR after passing through an Al filter having the thickness of 1 μm.
The dash-dot line shows the energy of the L-edge of the radiation absorption for aluminum (EL=72.6 eV).
After the DTR passes through an Al filter, the radiation yield will be suppressed for quanta having energy Eg> EL.
Curves 1a, 2a, 3a and 4a show angular distributions of BTR taking absorption in the Al filter into account and are multiplied by factor of 5.
Curves 1a, 2a, 3a and 4a in Fig. 5 show the angular distributions of the BTR after passing through an Al filter having the thickness of 1 μm.
The dash-dot line shows the energy of the L-edge of the radiation absorption for aluminum (EL=72.6 eV).
After the DTR passes through an Al filter, the radiation yield will be suppressed for quanta having energy Eg> EL.
Online since: November 2010
Authors: J. Dutchaneephet, Sorapong Pongkrapan, Pisutti Dararutana, Krit Won-In, N. Sirikulrat
El-Diasty et al.: Journal of Applied Physics, Vol. 100 (2006), p. 093511
Costa et al.: J.
Haouri et al.: J.
Murata et al.: J.
El-Diasty: Current Opinion in Solid State and Materials Science, Vol. 10 (2006), p. 217-229.
Costa et al.: J.
Haouri et al.: J.
Murata et al.: J.
El-Diasty: Current Opinion in Solid State and Materials Science, Vol. 10 (2006), p. 217-229.
Online since: August 2015
Authors: Van Diem Thi, Mourad Khelifa, Mohammed El Ganaoui, Yann Rogaume
Numerical analysis of laminated veneer lumber panels in fire
THI Van Diem1,2, KHELIFA Mourad1,*, EL GANAOUI Mohammed2, ROGAUME Yann1
1 University of Lorraine, LERMAB, EA 4370, 27 rue Philippe Séguin, 88026 Epinal Cedex, France
2 University of Lorraine, LERMAB, EA 4370, IUT of Longwy, 54400 Cosnes et Romain, France
* mourad.khelifa@univ-lorraine.fr (M.
An early model for wood charring was given by Bamford et al. [7].
Fredlund [9] and R.M Knudson et al. [10] are given in Figs.1.
Khelifa, A.Khennane, M.El Ganaoui, Y.Rogaume.
An early model for wood charring was given by Bamford et al. [7].
Fredlund [9] and R.M Knudson et al. [10] are given in Figs.1.
Khelifa, A.Khennane, M.El Ganaoui, Y.Rogaume.