Search results

Acknowledgments The authors are grateful to the financial support provided by Natural Science Foundation of China (No. 50706028) and Shanghai Leading Academic Discipline Project (No.S30503).
Journal of Refrigeration. 2008,29(3):18-23 [3] Sandrine Marinhas, Anthony Delahaye, Laurence Fournaison.
International Journal of Refrigeration , 2007，30(5):758-766
Chemical Engineering Science. 2008, 63(13):3551 – 3559
Journal of Chemical Industry and Engineering.2008,59(6):1545-1550

For comparing, the beam model according the document [6], and its geometric and material parameters are listed as the following: Density 33 /1086.7 mkg×=ρ , Young's modulus GpaE 210= , Beam height mh 1= Beam thickness mb 5.0= , Beam length mL 50= , moving load K�P 10= The response of the beam under a moving load is calculated by code A�SYS, which is also a function with the different location of the load.
Acknowledgment This study was supported by the Key Natural Science Research of Guangdong Province,China P.R (Grant No. 05Z003), the Project of tackling key problem of Guangdong Province, China P.R (Grant No. 2006B12401008) and the National Natural Science Foundation of China (Grant No. 10672067).
Journal of Solids and Structures.
Journal of Solids and Structures.
Mahmoud, Journal of Rail and Rapid Transit.

Acknowledgements This work was financially supported by The National Natural Science Foundation (51275063).
Science and Technology Innovation Heraid (2011), p. 23.
Chinese Journal of Mechanical Engineering Vol. 39 (2003), p. 38.
Journal of China University of Mining & Technology Vol.38 (2009), p. 240.
Journal of Chong Qing University Vol. 32 (2009), p. 299.

Journal of Management, 17(1), 1991.99−120
Organization Science , . 12( 6) 2001
Advanced Management Journal Spring. pp. 1996.11-15
Decision Sciences, 29(3). 1998
International Journal of Project Management . 3(4): 2003.243-250

The wide range of experimental data on creep of crystalline materials indicates the complex nature of the process.
Beribeche, Effect of Prior-Heat Treatments on the Creep Behavior of an Industrial Drawn Copper, World Journal of Condensed Matter Physics, 2(4) (2012) 241-245
Ji, Heat Treatments Effect on the Mechanical Properties of Industrial Drawn Copper Wires, Advanced Materials Research, 811 (2013) 9-13
Computational Materials Science, 19 (1-4) (2000) 267-274
Kulaeva, Modeling of temperature and rate dependence of the flow stress and evolution of a deformation defect medium in dispersion-hardened materials, Bulletin of the Russian Academy of Sciences: Physics 74 (11) (2010) 1527-1531

Mechanical properties of materials for tension sample are presented in Table 1.
Mechanical properties of a shear sample material are defined in Tab. 2.
[7] Šimčák, F., Kalina, M., Orečný, M., The Verification of Fixture for Shear Load with Optical Method ESPI, American Journal of Mechanical Engineering, 1 (2013) 180-184
Composites part A, Applied Science and Manufacturing. 2011, 42. s. 111-121
P., Grasso, M., Penta, F., Pinto, P., On the mechanical characterization of materials by Arcan-type specimens, Science Direct, Engineering Fracture Mechanics, Volume 78, s. 1729-1741. 2011

Additionally, the attenuation of electromagnetic wave and the non-homogeneity of sub-surface materials give rise to a reduction in quality of the radar image.
In all cases, water content ratio of sand for sub-surface material is 1.7%.
In the case of voids existed deeply under concrete slab, as shown in Fig. 3(b) and 9, it is necessary for contrast enhancement of the radar image, as pre-process, to apply the proposed method because reflections from the void are weakened by the attenuation effect, mainly from slab thickness, void depth and the change of electromagnetic properties within non-homogeneity materials.
Title of Publication (to be inserted by the publisher) In the case of detecting voids under concrete slab, it is necessary for contrast enhancement or noise filtration of radar image, as pre-process, to apply the proposed method because reflections from voids are weakened by the attenuation effect from void depth, thickness of slab and the change of electromagnetic properties within non-homogeneity materials.
Nondestructive Test for Concrete Structures Using Radar (3), Journal of Institute of Industrial Science, University of Tokyo, Vol. 48, No. 5, 1996

Xiong b Department of Materials Science and Engineering, Xiamen University, Xiamen 361005, China b zxxiong@xmu.edu.cn Keywords: Rare earth phosphor; Ca0.85(W1-xMox)O4:Eu0.15; Luminescence Abstract.
Experimental Raw materials.
Optical Materials, Vol. 4(2006), p. 120
Journal of Alloys and Compounds, Vol. 10(2006), p. 488
Grabmaier: Luminescent Materials (Verlag, Berlin, Germany, 1994), p. 41.

Experiment Materials.
Polypropylene, T30S, Guangzhou Maoming Petrochemical Company; nano-TiO2, rutile, 20nm, New Material Co., Ltd.
And then adding PP to the masterbatch to prepare composite materials in nano-TiO2 mass rate of 1%, 1.5%, 2% and 2.5%, respectively recorded as PP-1, PP-1.5, PP-2 and PP-2.5.
Chen: Polymer Materials Science and Engineering China Vol. 23 (2007), p.159-162 [5] H.
Zhang: Journal of Polymer Science China Vol. 42 (2004), p. 1181-1191 [8] B.

Study on Preparation and photoluminescence performance of High-directional ZAO Nanorod Arrays Yanglin Liu1,2,a , Xuechen Duan 1,b, Yanyan Liu3,c 1School of Material Science and Engineering, Central South University,Changsha,China 2Changsha Environmental Protection College, Changsha,China 3College of Science and Engineering, Jinan University, Guangzhou,China aLYL9909@126.com,bxc_d@vip.tom.com,c124917785@qq.com Key words:Al-doped zinc oxide (ZAO);nanorod arrays;thin film;preparation; photoluminescence.
Raw materials ZAO Precursor Into the reactor Hydrothermal reaction Separation of reaction solution Low-temperature drying ZAO nanorod arrays ZAO seed layer Figure 1 Preparation process diagram of ZAO array films Dissolve Mixing Figure 2 XRD pattern of ZAO array films With 5% AI-doping concentration 3.2 Impact of Aluminum Doping on the Shape of Nanorod Arrays Figure 3 is the SEM image of ZAO seed layer and nanorod arrays: granules of ZAO seed layer are densely arranged and evenly distributed, with an average size of about 45nm.
Materials Letters, 2005, 59: 3620~3625
Journal of Physical Chemistry B, 2006, 110: 20263-20267
Nature Materials, 2005, 4: 455-459