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Online since: November 2011
Authors: Rattanakorn Rawangkul, Wanchai Yodsudjai, Weerapol Namboonruang, Nutthanun Suphadon
1 Year Long Term on Strength Properties of Pozzolanics
Local Soil Bricks
W.
The significant property of fly ash is increasing the durability of materials [1,2].
Its surface is rough as shown in figure 1(a).
Figure 1(b) shows the shape and particle group of Mae-moh fly ash.
(a) (b) Fig.1.
The significant property of fly ash is increasing the durability of materials [1,2].
Its surface is rough as shown in figure 1(a).
Figure 1(b) shows the shape and particle group of Mae-moh fly ash.
(a) (b) Fig.1.
Online since: June 2015
Authors: M.R. Sahar, Sib Krishna Ghoshal, Siti Aishah Jupri
Ghoshal3, c
1, 2, 3Department of Physics, Faculty of Science,
Universiti Teknologi Malaysia, 81310 Johor Bahru, Johor.
The glass sample is cut in the dimension of 1 cm x 1 cm x 1 cm using diamond cutter.
Table 1 Optical parameters of Eu3+ doped lithium tellurite glass.
References [1] B.J.
Lin, Journal of Alloys and Compounds 479 (2009) 352-356
The glass sample is cut in the dimension of 1 cm x 1 cm x 1 cm using diamond cutter.
Table 1 Optical parameters of Eu3+ doped lithium tellurite glass.
References [1] B.J.
Lin, Journal of Alloys and Compounds 479 (2009) 352-356
Online since: January 2014
Authors: Widyastuti Widyastuti, Hosta Ardhyananta, Endah Kharismawati, Mochammad Zainuri
The stirring time was varieties by 1, 2, 3 hours.
Stirring time was varieties for 1, 2, and 3 hours.
Particle was agglomerated as Fig 1(a) for pH 7,5, but particle appear porous as Fig 1(b).
References [1] Ataie, A., S.E.
Yanwei, Journal of Alloys and Compounds 479 (2009) : 863-869
Stirring time was varieties for 1, 2, and 3 hours.
Particle was agglomerated as Fig 1(a) for pH 7,5, but particle appear porous as Fig 1(b).
References [1] Ataie, A., S.E.
Yanwei, Journal of Alloys and Compounds 479 (2009) : 863-869
Online since: February 2006
Authors: Chang Gil Lee, Geun Tae Bae, Dong Yim Chang, Sung S. Park, Nack Kim
Bae
1,a, S.S.
Table 1.
Summary 1.
Forum Vol. 475-479 (2005), p. 521
Forum Vol. 475-479 (2005), p. 457
Table 1.
Summary 1.
Forum Vol. 475-479 (2005), p. 521
Forum Vol. 475-479 (2005), p. 457
Online since: April 2014
Authors: Guang Su Li, Jie Ding
Due to change the formula of the plating solution, the layer will have good rigidity after heat treatment[1-3].
All the formulas are listed in Table 1 to table3.
Results and discussion The influence of NiSO4·6H2O concentrations in plating solutions to the plated layer thickness and surface brightness are listed in table 1.From table 1, when the concentration of NiSO4·6H2O was 320g/L, the plating speed was quickest.
130 381 432 812 683 3 11.155 105 293 431 478 581 4 13.474 90 299 388 450 525 5 10.637 85 298 418 586 653 6 2.125 130 375 410 893 738 7 4.665 120 355 479 752 782 8 10.651 117 304 407 512 600 9 14.212 75 293 362 457 513 10 12.157 73 296 445 535 621 Fig.1 Abrasion width change of the plated layers by different testing time Fig.2 The layer surface of sample 6 before and after 200, 400, 600oC heat treatment (200×) Fig.3 XRD pattern of sample 6 before and after 200, 400, 600oC heat treatment From table 3, after 1h 400oC heat treatment the layers’ rigidity of sample1, sample2 and sample6 were over 800HV and sample 7 arrived 782HV after 1h 600oC heat treatment.
References [1] K.P.
All the formulas are listed in Table 1 to table3.
Results and discussion The influence of NiSO4·6H2O concentrations in plating solutions to the plated layer thickness and surface brightness are listed in table 1.From table 1, when the concentration of NiSO4·6H2O was 320g/L, the plating speed was quickest.
130 381 432 812 683 3 11.155 105 293 431 478 581 4 13.474 90 299 388 450 525 5 10.637 85 298 418 586 653 6 2.125 130 375 410 893 738 7 4.665 120 355 479 752 782 8 10.651 117 304 407 512 600 9 14.212 75 293 362 457 513 10 12.157 73 296 445 535 621 Fig.1 Abrasion width change of the plated layers by different testing time Fig.2 The layer surface of sample 6 before and after 200, 400, 600oC heat treatment (200×) Fig.3 XRD pattern of sample 6 before and after 200, 400, 600oC heat treatment From table 3, after 1h 400oC heat treatment the layers’ rigidity of sample1, sample2 and sample6 were over 800HV and sample 7 arrived 782HV after 1h 600oC heat treatment.
References [1] K.P.
Online since: April 2016
Authors: Shu Yu Zhong, Pei Song Tang, Ji Qi Jiang, Hai Shao Ye, Qian Yang
Fig. 1 XRD pattern of LaVO4
Morphology Analysis of LaVO4.
There were four characteristic peaks of the 440 cm-1, 795 cm-1, 1426 cm-1 and 3406 cm-1 in the Fig. 4.
The peaks around 3406cm-1 and 1626cm-1 were due to the O-H stretching vibrational mode of absorption. 795 cm-1 and 440 cm-1 should be the vibration peak of Fe-O and V-O bond.
Reference [1] S.
Jinénez-Mier: J Alloy Compd, Vol.479 (2009), p.511
There were four characteristic peaks of the 440 cm-1, 795 cm-1, 1426 cm-1 and 3406 cm-1 in the Fig. 4.
The peaks around 3406cm-1 and 1626cm-1 were due to the O-H stretching vibrational mode of absorption. 795 cm-1 and 440 cm-1 should be the vibration peak of Fe-O and V-O bond.
Reference [1] S.
Jinénez-Mier: J Alloy Compd, Vol.479 (2009), p.511
Online since: February 2009
Authors: Chun Xu Pan, Fu Fang Zhou, Bao Gai Zhai, Zhuo Ran She, Yuan Ming Huang
Figure 1 shows the typical I-V curves of the polypyrrole palettes 1, 4, 5-8,
respectively.
As described in Ref. [9], the slopes of the curves were calculated be 0.18, 0.18, 0.18, 0.52, 1.33, 16.3, 0.09 and 1.10 for the samples 1-8, and the conductivity of the eight samples were obtained to be 607, 479, 468, 135, 83, 10, 1680 and 251 S/m, respectively.
Fig. 1.
Particle size distributions of the powders of 1-8.
References [1] Y.M.
As described in Ref. [9], the slopes of the curves were calculated be 0.18, 0.18, 0.18, 0.52, 1.33, 16.3, 0.09 and 1.10 for the samples 1-8, and the conductivity of the eight samples were obtained to be 607, 479, 468, 135, 83, 10, 1680 and 251 S/m, respectively.
Fig. 1.
Particle size distributions of the powders of 1-8.
References [1] Y.M.
Online since: February 2008
Authors: Qing Zhang, Jun Ting Luo, Hong Bo Li
Physical properties of all powders
are shown Table 1.
Fig.1 shows the value of friction coefficient as a func- tion of wear time for four types of samples.
When sliding, after a certain time, the friction coefficient increases sharply from o.1 to maximum.
References [1] I.W.
Vol.475-479 (2004), p.2987
Fig.1 shows the value of friction coefficient as a func- tion of wear time for four types of samples.
When sliding, after a certain time, the friction coefficient increases sharply from o.1 to maximum.
References [1] I.W.
Vol.475-479 (2004), p.2987
Online since: August 2013
Authors: Hui Hua Zhang, Dong Feng Zhou
Ang and Clements [1] applied the boundary integral method to examine the effect of holes on the crack tip stress intensity factors in anisotropic materials.
Crack Void (a) (b) Fig. 1.
The relaxation modulus in Eq. 1 for this material is (10) When modeling, the dimensions in Fig. 2 are chosen as: the plate width , the crack length and the void radius .
References [1] W.T.
A/Solids 18 (1999) 465-479
Crack Void (a) (b) Fig. 1.
The relaxation modulus in Eq. 1 for this material is (10) When modeling, the dimensions in Fig. 2 are chosen as: the plate width , the crack length and the void radius .
References [1] W.T.
A/Solids 18 (1999) 465-479
Online since: June 2014
Authors: Atirat Maksuwan
The discussion is found in figure 69 on pages 108 of QED [1].
The physical picture of research Feynman’s so-called “polarization-free photon” is technically called “Klein-Gordon particles” of the zero mass propagators [1].
References [1].
Particles, sources and fields vol. 1 (1970a).
Foundations of Physics, 19(5), 479-504.
The physical picture of research Feynman’s so-called “polarization-free photon” is technically called “Klein-Gordon particles” of the zero mass propagators [1].
References [1].
Particles, sources and fields vol. 1 (1970a).
Foundations of Physics, 19(5), 479-504.