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Beam length is 600mm, and the material of beams is the same as each other.
Dimension parameters and material attributes of beams and cables are shown in Table 1.
Acknowledgements This project is supported by Key Program of National Natural Science Foundation of China (No.50935002) and the Program of Introducing Talents of Discipline to Universities (No.
Tsujigata: 42th AIAA/ ASME/ ASCE/ AHS/ ASC Structures, Structural Dynamics, and Materials Conference and Exhibit (Seattle, WA, United States, 2001), pp. 2222-2227
Tsujihata: Journal of Spacecraft and Rockets, Vol. 43 (2006), pp. 780-787

The other hand, Ti-Ni-Zr alloy was well known high temperature shape memory material [1-2].
[2] Bertheville, B., Journal of Alloys and Compounds, Vol. 398, No. 1-2 (2005), pp.94-99
K., Materials Characterization, Vol. 41 (1998), pp. 151-162
,Material Science and Engineering, A, Vol.438-440 (2006), pp. 675-678
and Yoshimi, Y., Material Transactions, Vol 47, No.11 (2006), pp. 2867-2870

Effect of deashing treatment on the coal structure and surface groups Shixiong HAO a, Xingyong LIU b and Zuxiao YU c College of Materials and Chemical Engineering, Sichuan University of Science and Engineering, Zigong, China ashxionghao@126.com, bxingyong.l@163.com, cyuzuxiao@126.com Keywords: Coal, Deashing treatment, X-ray photoelectron spectroscopy, Texture.
Experimental 2.1 Materials The raw coal studied was from Datong (China).
Pevida, Ammoxidation of carbon materials for CO2 capture, Appl.
Zhao, Manganese promoting effects on the Co-Ce-Zr-Ox nano catalysts for methane dry reforming with carbon dioxide to hydrogen and carbon monoxide, Chemical Engineering Journal, 170 (2011) 457-463

3D-Modeling and Numerical Analysis of Fracture Behavior in AFM-Specimen on Mixed-mode I-II Loading Condition Qing-fen Li 1,a, Li Zhu 1,b, Guo Jin 2, Xiu-fang Cui 2 1College of Mechanical and Electrical Engineering, 2College of Material Science and Chemical Engineering, Harbin Engineering University, Harbin 150001, China aqingfli@yahoo.com.cn, bzhuli0712@hrbeu.edu.cn Keywords: 3D-modeling; numerical analysis; all fracture modes (AFM) specimen; mixed-mode fracture; strain energy release rates (SERRs) Abstract.
Introduction In practical engineering, mixed mode fracture is one of the most common failure forms of structure and building materials.
The material parameters are chosen as follows: Young’s modulus E =N/mm2 and Poisson’s ratio n =0.3.
Dhondt: Key Engineering Materials, vol. 251-252 (2003), p. 209-214 [3] Erdogan, F., Sih, G.
C: Journal of Basic Engineering, vol.85 (1963), p.519-527 [4] Richard, H.

Characteristics of the Test Samples Material.
Publicated in: Advanced Material Research 2013
Publicated in: Advanced Material Research
In: Applied Mechanics and Materials (Volume 300 – 301), pp. 860-869.
Geometrically Non-linear Finite Element Reliability Analysis of Steel Plane Frames With Initial Imperfections, Journal of Civil Engineering and Management, 18(1), 2012, pp. 81-90, ISSN 1392–3730 print / ISSN 1822–3605 online

Imai2,c 1 Graduate School of Science and Technology, Nagasaki University, Bunkyo-machi, Nagasaki 852-8521, Japan 2 Faculty of Engineering, Department of Mechanical Systems Engineering, Nagasaki University, Bunkyo-machi, Nagasaki 852-8521, Japan a s-aki@nagasaki-u.ac.jp, btoyota@survic.mech.nagasaki-u.ac.jp, cimai@nagasaki-u.ac.jp Keywords: Compressive Fracture, Asperity, Roughness, Crack Path Simulation, Body Force Method Abstract.
Introduction One of the most characteristic points of brittle or quasi-brittle materials is its strength against compression.
In general, it is known that the endurance against compression is several to dozen times that of against tension for many brittle materials.
Although brittle materials can resist considerable compressive stress, cracks may propagate to lead a failure under excessive compression.
[4]Nisitani, H., Journal of JSME, Vol.70, No. 580, pp.627, 1967.

Kurz, International Materials Reviews, Vol. 39 (1999) p.49 [5] S.
Mathiesen et al., Metallurgical and Materials Transactions B, Vol. 33B (2002) p. 613 [7] H.
Okamoto, Journal of Phase Equilibria, Vol. 19 (1998) p. 86 [8] Y.
Du et al., Materials Science and Engineering A, Vol.

Introduction With the development of science and technology, the realization method of remote education is ever-evolving from the initial correspondence teaching by mail or email to teaching through radio and television and then to the current Internet-based digital learning mode [1].
Teachers release teaching materials of the course, including teaching courseware, reference materials, syllabus, schedule of the course, teaching video, assignments, teaching log, etc..
Cairngorm, Spring and Hibernate open source framework, MVC, DTO and Singleton design mode are used to realize《Mechanics of Materials》course learning system.The realized functions operate well in the test.
Journal of Beijing University of Posts and Telecommunications(2010) [5] Yu Shengquan.

In the third group, the exhaust manifold surface is coated by compound silicate insulation materials.
The materials make the internal temperature not to be distributed to the surface, so the surface temperature is controlled within the required 150 ℃.
The method of heat insulation which means coating the exhaust mainfold by special material will make the surface temperature not exceed 150℃.
While the heat preservation material price is so high that the manufacturing cost will rise.
Journal of Shijiazhuang Railway Institute, Vol.12, pp.77, sep. 1999.

Numerical Study on the Fluctuation of Free Surface in the Vacuum Vessel of RH-TB Fengsheng Qi1, a, Yu Jiang1, b, Liu Yang1, c, Fang Wang1, d, Baokuan Li1, e 1School of Materials and Metallurgy, Northeastern University, Shenyang 110819, China aemail: qifs@smm.neu.edu.cn, bemail: happyforever.jj@163.com, cemail: tianjiao_1584@163.com, demail: wangfang@smm.neu.edu.cn, eemail: libk@smm.neu.edu.cn Key words: RH-TB, refining, vacuum vessel, free surface Abstract.
A three-dimensional mesh was generated over the entire domain as shown in Fig.2 and the details of geometry and parameters of materials used in the simulation are given in Table 1 and Table 2.
Table1 The details of geometry Item detail（m） Vacuum vessel: Diameter/Height 1.8/3 Oxygen lance: Diameter /Depth 0.14/1.8 Snorkel: Diameter/ Height/Center distance 0.45/0.5/1.2 Table2 Parameters of materials used in the simulation Item density（kg/m³） viscosity（Pa·s） Oxygen 1.2999 1.919×10-5 Slag 3490 0.03 Melt 6940 0.0051 Boundary condition and Numerical details No slip boundary condition was used at the oxygen lance, up-leg snorkel, down-leg snorkel, vacuum vessel walls.
Acknowledgements This work is supported by National Natural Science Foundation of China, granted NO. is 51004029.
Saito: ISIJ International Vol.35(1995), P. 1452 [10] X．Li, X．P．Liang, Y．Jin, H．Pan： The Chinese Journal of Process Engineering Vol.9 (2009), P. 324 [11]P.Anil KISHAN and Sukanta K.PASH: ISIJ International Vol. 49(2009), P. 495