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Online since: March 2016
Authors: Xiu Yun Meng, Wei Zhong Zhang, Yong Sheng Wu
Fig. 1: Composition of the cable-net reflector.
Table 1: Structural parameters of the reflector.
They were also evaluated from the disturbed node (1) to the observed nodes (1, 19, 27, 35).
References [1] Thomson, M.W.
Advanced Mechanical Design, Pts 1-3, 2012. 479-481: p. 1490-1494
Online since: June 2012
Authors: Xiu Li, Yin Shun Wang, Yang Rui Zhang
Fig.1.
The main parameters of the DP are shown in Table 1.
References [1] O.
Supercond. vol. 10, no. 1, pp. 482-485, March 2000
Technol. vol. 20, no. 5, pp. 479-484(6), May 2007.
Online since: May 2014
Authors: Thapanun Sudhawiyangkul, Songmoung Nundrakwang, Don Isarakorn
The proposed energy harvester [15] used piezo-buzzer with 2.6 kHz resonant frequency as shown in Fig.1 (a).
Table 1 lists the current consumption of the sensor node.
In this research, the LTC3588-1 is set to have the operative voltage range at 3.6V-5V.
Reference [1] V.
[14] Jianmin Hou and Yi Gao, “Greenhouse Wireless Sensor Network Monitoring System Design Based on Solar Energy”, 2010 International Conference on Challenges in Environmental Science and Computer Engineering, pp. 475-479, 2010
Online since: April 2006
Authors: Jumpei Ogawa, Takashi Fukuda, Tomoyuki Kakeshita, Mi Seon Choi
Stability of the B2-type structure of Ti-Ni-Fe and Ti-Ni-Co shape memory alloys Mi-Seon Choi 1,a , Jumpei Ogawa1,b , Takashi.
A negative temperature dependence in the electrical resistivity [1-3], diffuse scattering near 1/3[110] or streaks in the electron diffraction pattern [4,5], softening in the TA2 phonon branch near 1/3[110] [6,7] etc. appearing in the parent phase of Ti-Ni alloys are considered to be premartensitc phenomena.
Figure 1 shows the cooling curve of DSC Fig. 1 DSC cooling curves of (a) Ti-(50-x)Ni -xFe, and (b) Ti-(50-x)Ni-xFe alloys.
References [1] T.
Forum Vol. 475-479 (2004), p. 1977 [16] J.
Online since: September 2015
Authors: Elena Avtokratova, Oleg Sitdikov, Oksana Mukhametdinova, M.J.N.V. Prasad, Michael Markushev, Bhagwati Prasad Kashyap, S.V.S. Narayana Murty
Tensile tests were carried out on Instron 1185 universal testing machine in the temperature range of 350-520°C and strain rates of 10-3-10-1 s-1.
Fig. 1.
EBSD maps from the samples gauge with highest elongations to failure: (a) ECAP (δ=2570%, 520oС, 1.4×10-2s-1); (b) ECAP and cold rolling (δ=3030%, 520oC, 1.4×10-2 s-1) contribution of grain boundary sliding to the total elongation may take place [1].
References [1] G.
Shin, Scripta Mater. 51 (2004) 479-483
Online since: February 2012
Authors: Yong Qiang Qin, Yu Cheng Wu, Xin Min Huang, He Bin Han, Jun Li Cao
Experimental results and discussion c d 1.
Microstructure b a f e Fig.1.
Conclusions 1.
References [1] X.F.
Journal of Alloys and Compounds, Vol.479(2009):303-306
Online since: September 2007
Authors: V. Dondur, R. Dimitrijević, A. Kremenović, B. Nedić
Weight percentage of Sr-hexacelsian was 94(1) %.
The exception is the band at 459 cm-1 for BAS, as well as bands at 365 and 635.5 cm-1 for SAS.
Table 3 Observed IR wave numbers in cm-1.
BAS BAS:Yb3+ ∆ν SAS SAS:Yb3+ ∆ν assignment 355 355.5 0.5 365 358.5 6.5 394.5 394.5 0 391.5 393.5 2 υ2 SiO4[25] 459 466.5 7.5 475.5 479 3.5 482 482.5 0.5 498 499 1 570.5 571 0.5 565.5 564.5 1 υ4 SiO4[25] 638 636.5 1.5 635.5 642.5 7 672 671 1 671.5 671.5 0 A B Figure 5.
References [1] F.
Online since: July 2015
Authors: Michiharu Tabe, Takeshi Mizuno, Daniel Moraru, Arup Samanta, Takahiro Tsutaya, Yuki Takasu
The basic SOI-FET device structure is shown in Fig. 1(a).
Fig. 1.
Illustrations of the basic doping steps, critical for these two types of devices, are shown in Figs. 1(d) and 1(e).
References [1] H.
Lett. 6 (2011) 479
Online since: June 2014
Authors: Athipong Ngamjarurojana, Apichart Limpichaipanit, Komsanti Chokethawai, Khem Chirapatpimol, Ladapak Chumprasert
Curves 1-5 represent different soaking time of the function, (1) 1200-2h; (2) 1200-4h; (3) 1200-6h; (4) 1200-8h; (5) 1200-10h.
The temperature dependences of the dielectric constant in Fig. 5 at 1 kHz for PLZT 8/40/60 PLZT ceramics.
Pr, Ps and Ec, have been extracted from the experimental data and given in Table 1.
References [1] Y.T.
Soc. 56 (9) (1973) 479-480
Online since: April 2013
Authors: Bao Jun Pang, Wei Zheng, Yong Chen
Experimental methods and results The general experimental test geometry is shown in Figure 1.
Table 1 presents the experimental test matrix, it gives details of specimen geometries and lay-ups.
Figure 1: General experiment test specimen geometry Table 1: Test matrix for the material characterization experiment test series Test Lay-up L (mm) w (mm) t (mm) g (mm) Tensile [0]8 250 15 1 56 [90]16 175 25 2 25 [±45]2S 250 25 1 50 Compression [0]8 140 12 1 64 [90]16 140 12 2 64 The tensile fiber-direction and transverse direction properties of composite were determined from tensile test on [0]8 specimens and [90]16 specimens, respectively, both of which were in accordance with ASTM standard D3039[14].
References [1] T.
Cheng, Compos: Part B, 33 (2002) 479–489
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