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Online since: January 2012
Authors: M. Haddad-Sabzevar, S. Sahebian, S.A. Hasheminezhad
Fig. 1.
In the early stage, the crystallization was ruled by nucleation, therefore U=0 and the activation energy EC(x=0) = En≃479 kJmol-1.
Conclusion 1.
The values of En and Eg is 479 kJmol-1and 309 kJmol-1, respectively.
References [1] T.L.
In the early stage, the crystallization was ruled by nucleation, therefore U=0 and the activation energy EC(x=0) = En≃479 kJmol-1.
Conclusion 1.
The values of En and Eg is 479 kJmol-1and 309 kJmol-1, respectively.
References [1] T.L.
Online since: May 2011
Authors: Gui Chang Liu, Li Da Wang, Dong Feng Xue
a
b
c
d
f
e
Fig. 1.
References [1] J.
Vol. 479 (2009)p.
Interfaces Vol. 1 (2009)p. 789
Vol. 479 (2009)p.
References [1] J.
Vol. 479 (2009)p.
Interfaces Vol. 1 (2009)p. 789
Vol. 479 (2009)p.
Online since: January 2016
Authors: Atirat Maksuwan
For example, suppose that we have a boundary between vacuum (media 1) and glass (media 2).
(1) If we integrate equation (1) with respect to x across between two regions, we conclude that
For the partial amplitude =1 is the most probability and correspond to the classical point of impact in classical ray on the junction surface.
References [1] E.
Foundations of Physics, 19 (1989) 479-504
(1) If we integrate equation (1) with respect to x across between two regions, we conclude that
For the partial amplitude =1 is the most probability and correspond to the classical point of impact in classical ray on the junction surface.
References [1] E.
Foundations of Physics, 19 (1989) 479-504
Online since: February 2006
Authors: M. Oida, S. Okuda, N. Saito, N. Isu, Masayuki Nogami, Kazuhiko Hattori
Oida
1, N.
Isu 1, S.
Okuda 1, N.
Nogami3,b 1 General Research Institute of Technology, INAX Corporation MInatomachi, Tokoname 479-8588, Japan 2 Development Office, Tile & Building Materials Division, INAX Corporation Kume, Tokoname 479-0002, Japan 3 Department of Materials Science and Engineering, Graduate School of Engineering Nagoya Institute of Technology, Gokiso-cho, Showa-ku, Nagoya 466-8555, Japan a kazu@i2.inax.co.jp, bnogami@nitech.ac.jp Keywords: Solidifing, Urban heat islands, Inorganic waste, Paving tile, Numerical simulation Abstract.
Table 1.
Isu 1, S.
Okuda 1, N.
Nogami3,b 1 General Research Institute of Technology, INAX Corporation MInatomachi, Tokoname 479-8588, Japan 2 Development Office, Tile & Building Materials Division, INAX Corporation Kume, Tokoname 479-0002, Japan 3 Department of Materials Science and Engineering, Graduate School of Engineering Nagoya Institute of Technology, Gokiso-cho, Showa-ku, Nagoya 466-8555, Japan a kazu@i2.inax.co.jp, bnogami@nitech.ac.jp Keywords: Solidifing, Urban heat islands, Inorganic waste, Paving tile, Numerical simulation Abstract.
Table 1.
Online since: March 2006
Authors: Hyoung Wook Lee, Hye Jin Lee, Sung Min Bae, Nak Kyu Lee, Seo Gou Choi, Duk Jae Yoon, Geun An Lee
The flow stress and the microstructure are shown in Fig. 1.
Table 1.
References [1] H.
Forum Vol.475-479 (2005), p.3235 [4] G.A.
Forum Vol.475-479 (2005) p.3247
Table 1.
References [1] H.
Forum Vol.475-479 (2005), p.3235 [4] G.A.
Forum Vol.475-479 (2005) p.3247
Online since: December 2010
Authors: Jian Zhang, Qiang Hua Li
System principle, buildup and explanation
The correlated demodulation principle based on the edge of FBG optical band-pass filter Matched FBG dynamic sensing and demodulation system is shown in Fig.1.
a) Sensing and Demodulation system b) Demodulation thoery schematic Figure 1.
Reference [1] AKIRAM, ISAMU Y.
SP IE, 2001, 4330 (479), 479~ 486 [2] Fan Dian, Jiang De-sheng, Mei Jian-cun.
Acta Photonic Sonica, 2006, 35(1), 118~121 [3] Li Dong-sheng, Sui Qing-mei, Cao Yu-qiang.
a) Sensing and Demodulation system b) Demodulation thoery schematic Figure 1.
Reference [1] AKIRAM, ISAMU Y.
SP IE, 2001, 4330 (479), 479~ 486 [2] Fan Dian, Jiang De-sheng, Mei Jian-cun.
Acta Photonic Sonica, 2006, 35(1), 118~121 [3] Li Dong-sheng, Sui Qing-mei, Cao Yu-qiang.
Online since: October 2014
Authors: Yong Guang Chen, Li Wan
Eq. (1) and (2) are the incompressible
Navier-Stokes equations.
time t rx,ry 0 5 10 15 20 25 30 0.5 0.5 0.55 0.55 0.6 0.6 0.65 0.65 0.7 0.7 0.75 0.75 rx ry Fig. 1: The evolution of rx and ry with µ = 0.1 and T0 = 10.0 time t rx,ry 0 5 10 15 20 25 30 0.5 0.5 0.55 0.55 0.6 0.6 0.65 0.65 0.7 0.7 0.75 0.75 rx ry Fig. 2: The evolution of rx and ry with µ = 1.0 and T0 = 1.0 The computational domain is [−1, 1] × [−1, 1], and we set ρ0 = 1.0 and µ = 0.1 throughout the domain.
References [1] Z.
Peskin, The immersed boundary method, Acta Numer. 11(2002) 479-517.[5] Z.
Lett. 17 (1992) 479-484
time t rx,ry 0 5 10 15 20 25 30 0.5 0.5 0.55 0.55 0.6 0.6 0.65 0.65 0.7 0.7 0.75 0.75 rx ry Fig. 1: The evolution of rx and ry with µ = 0.1 and T0 = 10.0 time t rx,ry 0 5 10 15 20 25 30 0.5 0.5 0.55 0.55 0.6 0.6 0.65 0.65 0.7 0.7 0.75 0.75 rx ry Fig. 2: The evolution of rx and ry with µ = 1.0 and T0 = 1.0 The computational domain is [−1, 1] × [−1, 1], and we set ρ0 = 1.0 and µ = 0.1 throughout the domain.
References [1] Z.
Peskin, The immersed boundary method, Acta Numer. 11(2002) 479-517.[5] Z.
Lett. 17 (1992) 479-484
Online since: May 2007
Authors: Shu Suo Li, Ya Fang Han, Ai Qin Liu, Lu Sun
Results and Discussion
Microstructure analyzed XRD patterns of cast
Nb-16Si-24Ti-6Cr-6Al-2Hf alloys doped with
various amount of B are shown in Fig.1.
Conclusions 1) The volume fraction of silicide increased due to the addition of B.
Reference [1]Bewlay B.P., Jackson M.R., Zhao J.C., Subramanian P.R..
Vols. 475-479(2005):717-720 [3]Y.P.
Vols. 475-479(2005):741-744 [4]E.Sarath K Menon etc.
Conclusions 1) The volume fraction of silicide increased due to the addition of B.
Reference [1]Bewlay B.P., Jackson M.R., Zhao J.C., Subramanian P.R..
Vols. 475-479(2005):717-720 [3]Y.P.
Vols. 475-479(2005):741-744 [4]E.Sarath K Menon etc.
Online since: April 2015
Authors: Ji Hun Park
This is possible either by metric reconstruction [1] or by actual size reconstruction [6].
A group of voxels replaced by a primitive shape Determine colors and other information for 3D primitive shape Fig. 1 Overview of 3D Mosaic in an input image sequence Overview of Our System Fig. 1 shows an overview of 3D mosaic given a set of input images.
Computing Surface Information Voxels are computed by phase (A) of Fig. 1 while surface deformation information is computed in phase (B).
References [1] R.
Mater. 479-480 (2013) 479-480
A group of voxels replaced by a primitive shape Determine colors and other information for 3D primitive shape Fig. 1 Overview of 3D Mosaic in an input image sequence Overview of Our System Fig. 1 shows an overview of 3D mosaic given a set of input images.
Computing Surface Information Voxels are computed by phase (A) of Fig. 1 while surface deformation information is computed in phase (B).
References [1] R.
Mater. 479-480 (2013) 479-480
Online since: September 2016
Authors: Sophia Arnauts, Dennis H. van Dorp, Frank Holsteyns, Graniel Abrenica
Atomic-layer-scale etching (vetch ~0.3 nm min-1) is observed for 0.1 mM H2O2 in H2O.
The etch rate of Ge in water increases to 3 nm min-1 for 3 mM H2O2.
(c) (d) Figure 1.
References [1] J.A. del Alamo, Nature¸479 (2011), 317
Pillarisetty, Nature, 479 (2011), 324
The etch rate of Ge in water increases to 3 nm min-1 for 3 mM H2O2.
(c) (d) Figure 1.
References [1] J.A. del Alamo, Nature¸479 (2011), 317
Pillarisetty, Nature, 479 (2011), 324