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Online since: June 2008
Authors: Jeong Soo Lee, B.J. Kim, Y.R. Son, J.O. Yun
Kim 1,a , Y.
Son 1,b , J.
Yun 1,c, J.
Lee 1,d 1 Hanjin Heavy Industries & Construction CO., LTD., 22-1, 4-Ga, Jungang-dong, Jung-gu, Busan, 600-814, Korea a bulkkot@hanjinsc.com , dwilson@hanjinsc.com, cjoyun@hanjinsc.com, dleejs@hanjinsc.com Keywords: Residual stress, Stress relief, Vibratory conditioning, Micro structure Abstract.
Forum Vol. 475-479 (2005), p. 3307 [2] A.S.M.Y.
Online since: November 2010
Authors: Richard Wuhrer, Wing Yiu Yeung, J. Qin, D. Zhang, Qiu Bao Ouyang, N.G. Booth, Sam R. Humphries
Wuhrer 1, N.G.
Booth 1 , W.Y.
Yeung 1 , Q.
Table 1.
Yeung, Materials Science Forum: 479 (2005) p.3501
Online since: December 2013
Authors: Ahmad Sahrim, Sinar Arzuria Adnan, Firuz Zainuddin, M.A. Nur Azni, Siti Nursyafiqah Samsudin, Hazizan Md Akil
They are also used in non-structural applications for cushioning, packaging and insulating purposes because of their energy absorbing properties and good vibration attenuation and thermal and acoustic insulations [1].
Figure 1: Compressive strength of pure PU and Al/PU-CNTs foam sandwich.
The compressive strength shows fluctuated values (Figure 1).
References [1] Liu, Q., Subhash, G., (2004).
Enhancement in thermal and mechanical properties of polyurethane foam infused with nanoparticles. (2008) Materials Science and Engineering A, 479, 213-222
Online since: June 2012
Authors: Ning Ning Liu
It proves a novel-framework for formulating numerical solutions to flow problems and brings certain advantages over conventional numerical methods [1].
The D1Q5 model is shown in Fig.1, the discrete velocity vectors are:, where,is the magnitude of velocity.
In this example, for the Lattice Boltzmann method, the single relax time=1, the space step=1cm and the time step=0.01min.
References [1].
Lett. 1992, (17):479-484
Online since: July 2013
Authors: Yu Du, Wen Hua Wu, Qian Jin Yue
FEM analysis of stud-less mooring chains According to the structure characteristics, mooring chain is composed of two types: stud chain and stud-less chain which shown in Figure 1.
Figure.1 Stud chain and Stud-less chain The simulated model is constructed by three chains.
The whole model is discretized by eight nodes solid element, as shown in Figure 2.The material parameters considered mooring chain is listed in Table 1.
References [1] Brown M G, Hall T D, Marr D G, et al, Floating Production Mooring Integrity JIP – Key Findings, C.
Marine Structures, 8(1995)451-479
Online since: November 2013
Authors: Alena Guseva, Natalia Gusakova
Development of the model for determining of the trophic status of shallow-water reservoir Gusakova N.V.1,a ,Guseva A.
Table 1.
References: [1] Gusakova N.V., Zhukevich O.V.
(Natural and exact sciences, technique) No.1, (87), 1979. – p.63. – Dep.
Marques/ Estuarine, Coastal and Shelf Science, Volume 60, Issue 1, May 2004, p/ 23-35
Online since: April 2007
Authors: Kai Zheng, Jian Xun, Shao Ze Yan
Piezoelectric stack actuator is the key part of the piezoelectric active member and its electro-mechanical properties will influence the control application of the active member in the truss structure [1-3].
Fig.1 shows a piezoelectric stack to be used in an active member for vibration control of the truss.
Displacement Sensor Nut PZT Stack Fixed End Sensor Targat Preload Spring Output Stem Ball Member Load Sensor Fig.1.
References [1] G.S.
Ephrahin: J Guidance, Control, and Dynamics. 1997, 20(3), pp.479.
Online since: September 2007
Authors: Jian Lu, Ke Wei Xu, Wu Tang, Long Jiang Deng
Surface Morphology, Crystal Orientation and Scratch Properties of Au/NiCr/Ta Multi-layered Metallic Films Wu TANG 1, a , Longjiang DENG1 , Kewei XU 2 and Jian LU 3 1 State Key Laboratory of Electronic Thin Films and Integrated Devices University of Electronic Science and Technology of China, Chengdu, 610054, China 2 State Key Laboratory for Mechanical Behavior of Materials Xi'an Jiaotong University, Xi'an, 710049, China 3 LASMIS, Université de Technologie de Troyes, 10010 Troyes Cedex, France a tang@uestc.edu.cn Keywords: Crystal orientation; Surface roughness; Scratch test; Metallic films.
The XRD spectrum of the films is shown in Figure.1.
References [1] S.
Schirrer: Thin Solid Films Vol. 479 (2005), P. 207 [6] Z.
Wadley: Thin Solid Films Vol. 471 (2005), P. 1 [9] Y.
Online since: June 2004
Authors: Sebania Libertino, Fabrizio Roccaforte, Lucia Calcagno, Paolo Musumeci, Francesco La Via, Ricardo Reitano, Alfonso Ruggiero, Marco Mauceri
A set of peaks (473-479 nm) related to carbon vacancies anneals at 600 °C, a second set (470 nm) is stable up to 900 °C and a third set (L1-473 nm and L2 - 480 nm) anneals starting from 400 °C.
High-energy irradiation can be used for lifetime control in bipolar devices and ion implantation for doping [1, 2].
Results and discussion In Fig.1 is plotted the trap concentration determined by DLTS spectrum of the as irradiated sample (solid line), which shows three peaks at temperatures of 230K, 275K, 365 K and a shoulder at 430 K.
We have investigated the thermal annealing of irradiated samples in the temperature range 200- 900 °C and the DLTS spectra plotted in Fig.1 show a change in the intensity of the different levels.
References [1] D.
Online since: November 2011
Authors: Fu Yuan Song, Yi Ma, Peng Zhang, Yue Jin Chen
From conservation of mass (1) The first law results as follows: (2) The second law results as follows: Fig.1.
Compressed air flows from the supply pipe through the setting valve 1 into the vortex board.
The result is that: (1) Exgery efficiency increases by increasing the inlet pressure up to =0.45MPa and it decrease at higher pressure.
References [1] Ranque G J.
Eng. 5(1950)473-479
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