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The overall microstructure of the hot-dip aluminized coating can be categorized into two domains: an outer Al-Si layer and an inner intermetallic layer with the chemical compositions of Fe-Al-Si.
The intermetallic layer formed underneath the Al-Si layer due to Al diffusion into the steel base metal.
These massive crystals are of Al–Fe–Cr–Si, where Al is in major quantity.
As the hot dipping bath of aluminum were containing Al 10 wt. % Si alloy, the deposited coating is in fact a eutectic lamellar structure of Al and Si.
Abd El-Lateef, V.M.

Al-Baghdadi2,b 1Department of Civil Engineering, College of Engineering, University of Baghdad, Baghdad, Iraq amreawa53@gmail.com, bhayder.baghdady@gmail.com Keywords: NSM; CFRP; flexural behavior; RC members; damaged RC members; Retrofitting.
Seracino et al. [5] conducted a series of tests on NSM-FRP to structural joints using CFRP strips.
Al-Saadi, A.
Al-Mahaidi, and J.
El-Hacha and S.H.

References [1] P.Nigam,G.Armour,IM.Banat,et al.
Technol.Vol.72(2000) ,p.219 [2] G.Mckay, M.El-Geundi, M.M.Nassar:Water research, Vol.24(1987),p.1513 [3] A.Khenifi, Z.Bouberka, F.Sekrance,et al.
:adsorption,Vol.13(2007),p.149 [4] V.K.Garg,M.Amita,R.Kumar,et al.
:Journal of Hazardous Materials.Vol. 144(2007),p.171 [7] S.Ricordel, S.Taha, I.Cisse,et al.
,Gonzo,l.F.Gonzo:Adsorp.Sci.Technol.Vol.23(2005),p.289 [9] S.J.Allen, Q.Gan, R.Mattews,et al.

Electrical Conductivity of Li2xZn2-3xTi1+xO4 Crystal Shin-ichi Furusawa, Yuusuke Koyama Department of Production and Science, Graduate School of Engineering, Gunma University 1-5-1 Tenjin-cho, Kiryu 376-8515, Japan furusawa@el.gunma-u.ac.jp Keywords: Lithium Zinc Titanate, Floating-zone Method, Crystal Growth, Crystal, Electrical Conductivity.
The crystal structure of LZTO is a spinel structure and the detail was analyzed by Hernandez et al. and Câmara et al. [7,8].
Câmara et al., International Journal of Quantum Chemistry Vol. 103, (2005) 580
[10] L.A.Lenonidov et al.: J.
[11] Z.Hong et al.: Electrochem.

It was shown in the work of Lee at el.[5] that stronger tumble during intake stage and the consequential turbulence levels at the time of ignition results in a faster flame development Figure 4.
Iwai, et al. (2002).
Huang, et al. (2005).
Bae, et al. (2007).
Nogi, et al. (2003).

Sun, et al: Chinese Journal of Lasers Vol.27 (2000), p. 756 [2] G.C.Lü, C.C.XU, H.D.Cheng: Chemical Industry and Engineering Progress Vol.27 (2008), p. 1284 [3] Z.Ma, Y.H.
Zhang , et al: Transactions of Materials and Heat Treatment Vol.28 (2007), p. 102 [4] R.G.
Wei, Q.L.Zhang, et al: Journal of Chinese Society for Corrosion and Protection Vol.20 (2000), p. 47 [5] H.F.
Wang, et al: Journal of Plasticity Engineering Vol. 13 (2006), p. 75 [8] Z.Ma, Y.H.
Zhang, et al: Transactions of Materials and Heat Treatment Vol. 28 (2007), p. 102

Taljsten [5], Malek et al. [6], Smith et al. [7] and Guo et al
Teng et al. [9], Yang et al. [10] used finite element analysis to simulate the interfacial stress.
References [1] Wight RG, El-Hacha R, Erki MA.

Box 11-8281, Riad El Solh 1107 2260 Beirut, Lebanon a maher.soueidan@univ-lyon1.fr, b olivier.kim-hak@univ-lyon1.fr, cgabriel.ferro@univ-lyon1.fr, d nada.habka@univ-lyon1.fr, ebnsouli@cnrs.edu.lb Keywords: Liquid phase, 3C-SiC, VLS, Growth kinetics, Germanium, µ-IR Abstract.
Similar thickness difference was obtained in the case of the VLS growth of SiC epilayers using Al-Si melts [11].
When comparing to Al-Si melts, 10 sccm of propane never involved the formation of a SiC crust on top of these melts [11].
The difference is most probably due to the fact that liquid Al-Si dissolves more C than liquid Ge-Si does (Al can dissolve much more C than Ge do).
The propane flux is fixed to 3 sccm. similar values of growth rates are found between the use of Ge-Si and Al-Si melts though the C solubility is several orders of magnitude higher in the latter case.

Alan Huber et al. [1] studied the influence of building width and orientation on plume issued from a stack in presence of building.
Marvoidis et al. [2] examined in scaled field and wind tunnel experiments the dispersion of atmospheric pollutant in the vicinity of isolated obstacles of different shape (cube, cylinder and taller obstacle) and orientation with respect to the mean wind direction.
Mahjoub et al. [3] study the flow field structure around three dimensional circular cylinders.
In another numerical work Mahjoub et al. [4] studied the dispersion of a pollutant around a twodimensional obstacle.
Aerod. (2006) [4] Mahjoub Said, N., Mhiri, H, El Golli, S., Le Palec, G., Bournot, P: Rev.

Also, McDaniel et al., 2010 [16] reported that a way to increase surface macrotexture is to use gradations with larger NMAS (nominal maximum aggregate size).
In the study conducted by Goodman et al. [6], experimental data confirmed that increased macro-texture may be achieved through use of gap-graded aggregates (increasing FM) increase of voids (VMA), use of coarser mixes (lower percentages of aggregates passing the 4,75 mm sieve) or reducing mix density (lower compaction efforts).
D’apuzzo et al. [11] proposed a research focused on the recalibration of the existing prediction models; authors found that the best fitting results were obtained by using VMA, Cc, Pb and P4,75 as independent variables, that seemed to be the most significant factors influencing surface macrotexture (for example, Mean Profile Depth, MPD and Estimated Texture Depth, ETD).
Finally, Miller et al., 2012 [19] and Wu et al., 2012 [20] focused on how texture affects friction.
Abd El Halim.