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Online since: December 2012
Authors: Othman Sidek, Yasir Hashim
Fig. 1(a) shows the Id–Vg characteristics with different lengths of the channel (L = 20, 30, 40, 60, 80, and 100 nm) at Vd = 1 V.
(a) (b) (c) Figure 1.
Effect of channel length on DIBL Fig. 1(c) shows the Id–Vg characteristics with different oxide thicknesses (Tox = 1, 2, 4, 6, 8, and 10 nm) at Vd = 1 V.
References [1].
Colinge & Jean-Pierre Colinge, Nature 479, 310–316 (17 November 2011)
(a) (b) (c) Figure 1.
Effect of channel length on DIBL Fig. 1(c) shows the Id–Vg characteristics with different oxide thicknesses (Tox = 1, 2, 4, 6, 8, and 10 nm) at Vd = 1 V.
References [1].
Colinge & Jean-Pierre Colinge, Nature 479, 310–316 (17 November 2011)
Online since: April 2015
Authors: Uda Hashim, A. Rahim Ruslinda, Mat Ayub Ramzan, M.K. Md Arshad, Saeed S. Ba Hashwan, M.F. Fatin
The result indicated that several peaks of the intensive bands at wavenumber of 3444.27cm-1, 1452.76cm-1, 1401.29cm-1, 1055.00cm-1, 793.90cm-1, and 479.72cm-1 were observed.
The peak at 3444.27cm-1 and 1452.7cm-1 were identified as O-H stretch and the in-plane O-H bending, respectively.
The intensity of the absorbance peak of O-H stretch in functionalized MWCNT at 3444.27 cm-1 was higher than raw MWCNTs indicating difference value of 1.01A and 2.22A respectively.
References [1] R.
Alloys Compd., vol. 501, no. 1, pp. 77–84, Jul. 2010
The peak at 3444.27cm-1 and 1452.7cm-1 were identified as O-H stretch and the in-plane O-H bending, respectively.
The intensity of the absorbance peak of O-H stretch in functionalized MWCNT at 3444.27 cm-1 was higher than raw MWCNTs indicating difference value of 1.01A and 2.22A respectively.
References [1] R.
Alloys Compd., vol. 501, no. 1, pp. 77–84, Jul. 2010
Online since: October 2007
Authors: Jong Gu Bae, Yo Sep Yang, Chan Gyung Park
Table 1.
For completing Fig. 1.
() 2 0 2 1.1215 cos 1 1.12 0.18sec (tan ) '2 ( 1 ) a xR Sin Uh d a E θ σθ θ ν × =++ − ∫Fig.2. comparisons of measured and calculated displacements: (a) A-1, (b) A-2, (c) B-1, (d) B-2, (e) B-3 and (f) B-4, respectively.
References [1] N.
Forum Vol. 475-479 (2005), p. 4125 [4] J.
For completing Fig. 1.
() 2 0 2 1.1215 cos 1 1.12 0.18sec (tan ) '2 ( 1 ) a xR Sin Uh d a E θ σθ θ ν × =++ − ∫Fig.2. comparisons of measured and calculated displacements: (a) A-1, (b) A-2, (c) B-1, (d) B-2, (e) B-3 and (f) B-4, respectively.
References [1] N.
Forum Vol. 475-479 (2005), p. 4125 [4] J.
Online since: April 2013
Authors: Wei Xu, Chang Hai Li
Langmuir model (1) and the Freundlich isotherm(2) were respectively expressed as follows [13,14]:
Qe = bQmax Ce/( 1+ KL Ce) (1)
ln Qe = lnKF + 1 /n lnCe (2)
The Qmax results from the Langmuir model at (288, 298 and308 K) were (28.51, 25.07, and 16.32 mg/g) , respectively, for As (V) (Table 1)
Freundlich constants were listed in Table 1.
References: [1] B.
B 76(1): 125–138 (2000)
Journal of Hazardous Materials B, 137: 464-479 (2006)
Desalination. 145( 1-3) : 293-298 (2002)
References: [1] B.
B 76(1): 125–138 (2000)
Journal of Hazardous Materials B, 137: 464-479 (2006)
Desalination. 145( 1-3) : 293-298 (2002)
Online since: February 2012
Authors: Weerapol Namboonruang, Nutthanun Suphadon, Prayoon Yong-Amnuai, Rattanakorn Rawangkul, Wanchai Yodsudjai
Table 1.
Figure 1.
However, the maximum thermal conductivity value at the ages of 28 and 180 days are 2.6512 W.mK-1 and 2.6998 Wm.K-1 for GVCM and 2.9845 W.mK-1 and 3.0025 W.mK-1 for LSC, respectively.
References [1] W.
,Vols. 261-263(2011) pp. 469-479, Trans Tech Publications, ttp, Switzerland, 2011 [4] Specification for interlocking block (non- bearing load type).TCPS:602-2547,2004, Bureau of Thai Industrial Standard, Bangkok
Figure 1.
However, the maximum thermal conductivity value at the ages of 28 and 180 days are 2.6512 W.mK-1 and 2.6998 Wm.K-1 for GVCM and 2.9845 W.mK-1 and 3.0025 W.mK-1 for LSC, respectively.
References [1] W.
,Vols. 261-263(2011) pp. 469-479, Trans Tech Publications, ttp, Switzerland, 2011 [4] Specification for interlocking block (non- bearing load type).TCPS:602-2547,2004, Bureau of Thai Industrial Standard, Bangkok
Online since: June 2013
Authors: Wan Qiang Hu
Some rolling technologies of explosive composite boards are listed in table 1.
Table 1 Some rolling technologies of explosive composite boards Num.
Figure 1 shows the wave on original bonding boundary becomes flatter along with the working rate increase.
(2) Solid solution processing technology is heating for 40 min at 1020℃, oil quenching Table 3 Mechanical Properties of nickel-titanium composite board at different states States Shear, MPa Peel, MPa Stretch Curve/Degree Sample Thichness/mm σb/MPa δ/% Inturn Excurvature Explosive 479 330 — — >180 >150 12.0 Hot Rolling — — 704 25.2 >60 >60 2.5 Cold Rolling — — 898 11.5 >20 >20 1.0 It is shown in table 2 and table 3 that, composite boards’ cutting and peeling strength data are commonly equivalent to the weaker one in component metals.
References [1] Huang Xingli, Li Pingcang, Hao Hongwei, et al.
Table 1 Some rolling technologies of explosive composite boards Num.
Figure 1 shows the wave on original bonding boundary becomes flatter along with the working rate increase.
(2) Solid solution processing technology is heating for 40 min at 1020℃, oil quenching Table 3 Mechanical Properties of nickel-titanium composite board at different states States Shear, MPa Peel, MPa Stretch Curve/Degree Sample Thichness/mm σb/MPa δ/% Inturn Excurvature Explosive 479 330 — — >180 >150 12.0 Hot Rolling — — 704 25.2 >60 >60 2.5 Cold Rolling — — 898 11.5 >20 >20 1.0 It is shown in table 2 and table 3 that, composite boards’ cutting and peeling strength data are commonly equivalent to the weaker one in component metals.
References [1] Huang Xingli, Li Pingcang, Hao Hongwei, et al.
Online since: March 2007
Authors: Lin Geng, Zhen Zhu Zheng, H.L. Wang
Geng
1,a, Z.Z.
Zheng 1,b , H.L.
Fig.1 X-Ray diffraction pattern of the as-sintered TiB+TiC/Ti composite.
The results are shown in Table 1.
N.: Materials Science Forum 475-479 (2005), p. 877-880 [9] S.
Zheng 1,b , H.L.
Fig.1 X-Ray diffraction pattern of the as-sintered TiB+TiC/Ti composite.
The results are shown in Table 1.
N.: Materials Science Forum 475-479 (2005), p. 877-880 [9] S.
Online since: February 2014
Authors: Wei Wu
Figure 1-a.
Time vs. speed Figure 1-b.
Time vs. torque Figure 1-c.
A phase current Figure 1-d.
[3] Ma Ruiqing, Liu Weiguo, Luo Guangzhao, and et al., “The Balanced Current Control of Dual-Redundancy Permanent Magnetic Brushless DC Motor”, Proceedings of the Eighth International Conference on Electrical Machines and Systems, vol.1, pp. 475-479, 2005
Time vs. speed Figure 1-b.
Time vs. torque Figure 1-c.
A phase current Figure 1-d.
[3] Ma Ruiqing, Liu Weiguo, Luo Guangzhao, and et al., “The Balanced Current Control of Dual-Redundancy Permanent Magnetic Brushless DC Motor”, Proceedings of the Eighth International Conference on Electrical Machines and Systems, vol.1, pp. 475-479, 2005
Online since: February 2011
Authors: Ning Liang, Bai Kun Wang, Hao Ding, Yun Xing Zheng
The chemical composition of the product was listed in Table.1.
XRD pattern of the product was shown in Fig. 1.
Fig. 1.
The bands at 1103 cm-1 and 795 cm-1 were assigned to the Si-OH dissymmetry and symmetry vibrations, respectively. 479 cm-1 band corresponded to the bending vibration of Si-O-Si [9,10].
References [1] Bingkun Xiong, Zhenhan Lin, XinminYang, Dongmin Jiang, Fangcheng Luo and Lingxiu Zhang: Prep.
XRD pattern of the product was shown in Fig. 1.
Fig. 1.
The bands at 1103 cm-1 and 795 cm-1 were assigned to the Si-OH dissymmetry and symmetry vibrations, respectively. 479 cm-1 band corresponded to the bending vibration of Si-O-Si [9,10].
References [1] Bingkun Xiong, Zhenhan Lin, XinminYang, Dongmin Jiang, Fangcheng Luo and Lingxiu Zhang: Prep.
Online since: September 2013
Authors: Yi Li, Yong Feng, Wen Yuan Wu, Zhen Yi Ji
References
[1] F.
Math Mech Res, Preprints, No.1, 1987, p 2–12
Vol. 24 No.1,2009, p 50-57 [10] Sasson A M.
Vo. 359 No.1,2006, p. 111-122
Appl. 96 (1983), p 463–479
Math Mech Res, Preprints, No.1, 1987, p 2–12
Vol. 24 No.1,2009, p 50-57 [10] Sasson A M.
Vo. 359 No.1,2006, p. 111-122
Appl. 96 (1983), p 463–479