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Online since: June 2011
Authors: Shou Cheng Ding
[7] Ko C C,Chen B M,Hu S Y,el al.
[8] Baoping Tang, Fabin Cheng, Shuren Qin, et al.
Online since: February 2008
Authors: Hikmet Ş. Aybar, Mohsen Sharifpur
The ensemble averaged two-phase flow equations using the interfacial forces between two phases were developed by many authors such as Arnold [10], Park [11], Arnold et al. [12], Antal [13], Drew and Lahey [14].
Drew et al. has continued their research in the ensemble averaging model and published their studies also [16-18].
EL-Wakil: Nuclear Energy Conversion (ANS Publication, USA, 1982)
Online since: April 2010
Authors: José Ignacio Pérez Calero, Cristina Alba Pérez Rendón
Aportación al estudio de los concentradores solares estáticos por refracción: aplicación a la Cuenca Baja del Guadalquivir.
[5] Miravete A. et al.
Refractoconcentradores solares: propuestas para la Arquitectura y el Urbanismo.
Online since: October 2004
Authors: Xiao Qing Huang, Yi Ping Liu, Ling Ling Hu, Li Qun Tang
(12) 0 2 4 6 8 10 0 10 20 30 40 Axi al st r ai n( %) Radial strain(%) Fig.3 Relations between radial strain and axial strain for aluminum foam with various initial density y=0.1972x 0 3 6 9 12 15 18 0 3 6 9 12 15 Ener gy obt ai ned by exper i ment s( J) Energy obtained by analysis(J) Fig.4 Comparisons of the energy absorption per initial unit volume between analysis and experiments y=1.1609x With the minimization condition 0 0 = r rm d dρ σ , optimized value of initial relative density can be deduced as: 0] )21)(1( )1[(] )21)(1( [ 1 2 0 2 0 1 1 1 0 0 0 = −− −−⋅+ −− ⋅ − = − −− r p n r nn r r p r rm C nJ n C nJ n Cn d d ρη υ ρ ρ ρη υ ρ σ
Table 1 0 10 20 30 0. 2 0. 25 0. 3 0. 35 0. 4 0. 45 I ni t i al r el at i ve densi t y( ) Final stress(MPa) 2t 3t 4t 5t 6t 2f 3f 4f 5f 6f Fig.5 Final stress occurring when a given deformation energy is absorbed by aluminum foam with various initial relative densities. (1) 2t, 3t, 4t, 5t and 6t are the testing results when energy equals to 2, 3, 4, 5, 6(MNm/m 3) separately. (2) 2f, 3f, 4f, 5f, 6f are the analytic results accordingly. 0rρ Table 1 Comparison of optimum initial relative density between analysis and experiments Given J [ ] 2 3 4 5 6 7 Optimum initial relative density obtained by Eq. (15) 0.240 0.273 0.300 0.322 0.341 0.359 Optimum initial relative density obtained by tests 0.234 0.303 0.303 0.331 0.352 0.361 3 m/mMN ⋅ lists the experimental extreme values of stress and those obtained by Eq. (15), they have a well agreement with each other.
Online since: December 2010
Authors: Eugene P. Yelsukov, O.M. Nemtsova, D.A. Petrov, Konstantin N. Rozanov, A.A. Chulkina, A.N. Maratkanova, S.F. Lomayeva
Itoh et. al: Applied Physics A: Mater.
Rozanov et.al: Phys.
El.
Online since: October 2017
Authors: Mohamed Kamari Halimah, I. Zaitizila, Farah Diana Muhammad, Nurisya Mohd Shah
According to Kupracz et al., at band 1075cm-1, asymmetric stretching vibration of Si-O-Si bonds will occur[7].
According to Rosmawati et al., 2008, the absence of sharp absorption peaks indicated of oxygen bonding in the glass network, for instance, the formation of nonbridging oxygen, changes the characteristics of the absorption edge[14].
El-Mallawany, Theoretical and experimental binary rare earth tellurite glasses, Infrared Phys. 29 (1989) 781–785 [7] P.
Online since: December 2011
Authors: Xin Li, Gui Chang Liu, Xue Wu Liu, Shen Chen, Guo Hua Chen
Since the original study of Padhi et al. lithium transition metal phosphate has been considered a promising cathode material for rechargeable lithium-ion batteries[1].
Carbon contents of these samples were all about 6% determined by vario EL cube infrared carbon sulfur detector(Eltar company, Germany).
[5] Yamada A, Hosoya M, Chung S C, et al.
Online since: May 2004
Authors: M.P. Seabra, Victor M. Ferreira, M. Avdeev, Andrei N. Salak
According to Reaney et al. [14], the presence and the change in the type of tilting for A 2+B 4+O3 complex perovskites was observed for t near to 0.965 and 0.985 (solid lines in Fig. 2).
(solid lines - boundaries according to Reaney et al [14]). 48 Title of Publication (to be inserted by the publisher) Microwave dielectric properties.
Reaney, E.L.
Online since: January 2013
Authors: Miftakhul Huda, Sumio Hosaka, Jing Liu, Zulfakri bin Mohamad, You Yin
a, Jing Liu1,b, Zulfakri bin Mohamad2,c, You Yin1,d, and Sumio Hosaka1,e 1School of Engineering, Gunma University 1-5-1 Tenjin-cho, Kiryu 376-8515, Japan 2Advanced Technology Research Center, Gunma University 1-5-1 Tenjin-cho, Kiryu 376-8515, Japan at12802274@gunma-u.ac.jp, bt11801376@gunma-u.ac.jp, czulfakri@gunma-u.ac.jp, dyinyou@ gunma-u.ac.jp, ehosaka@el.gunma-u.ac.jp Keywords: nano-patterning, self-assembly, nanodot, block copolymer, pattern-transfer Abstract.
Recently, Ion Bita et al. succeeded in forming BCP self-assembled nanodots with a diameter of 20 nm and a pitch size of 40 nm using PS-PDMS (Poly(styrene-b-dimethyl siloxane)) BCP and demonstrated the fabrication of long-range-order nanodot arrays by using electron-beam drawing template [3].
Akahane et al. demonstrated the formation self-assembled nanodots using PS-PDMS BCP as shown in Fig. 1 [4-7].
Online since: January 2012
Authors: Zhi Qin Chen, Wen Kui Li, Wei Jun Zeng, Yang Fei Chen, Hong Bo Liu
El-Wakil: Polym.
[6] Young Jeon Kim, Myung Il Kim, Chang Hun Yun, et al: J.
[8] L.B.Manfredi,O.de la Osa, N.Galego Fernandez, et al: Polymer Vol. 40 (1999) 867-3875
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