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Online since: August 2014
Authors: Dong Qiu, Wen Juan Dai
Acknowledgement
In this paper, the research was sponsored by the science and technology development project of Jilin Province (Project No. 20120420).
Journal of Iron and Steel Research International, 2013, 20 (6):7-12
Journal of Materials and Metallurgy, 2002, 1 (3): 182-184.
Journal of Iron and Steel Research International, 2013, 20 (6):7-12
Journal of Materials and Metallurgy, 2002, 1 (3): 182-184.
Online since: July 2014
Authors: Guo Liang Zhu
Experimental Research on the stress - strain curve of regional confined concrete under single axial press
Zhu Guoliang1, a
1GuiZhou Construction Science Research & Design Institude Co., Ltd, GuiZhou, China
aE-mail:zhuguoliang2371@sina.com
Keywords: The stress-strain curve; Regional confined; Ordinary confined; Single axial press; Constitutive relationship
Abstract: Regional confined concrete is base on confined concrete.
Introduction The composition and structure of concrete materials have property of non-homogeneous, non-linear and non-isotropic.
References [1] Cao X.M.Influence of Longitudinal Steel on Ductility of Square Columns under Axial Load,Journal of Guizhou university of technology,2002,31(5)
[6] Xi X.Y;Cao X.M.Research on Application of Confined Concrete in Beams, Journal of Guizhou university ,2003, 32(1)
Introduction The composition and structure of concrete materials have property of non-homogeneous, non-linear and non-isotropic.
References [1] Cao X.M.Influence of Longitudinal Steel on Ductility of Square Columns under Axial Load,Journal of Guizhou university of technology,2002,31(5)
[6] Xi X.Y;Cao X.M.Research on Application of Confined Concrete in Beams, Journal of Guizhou university ,2003, 32(1)
Online since: December 2012
Authors: Zhi Qun Cheng, Li Wei Jin, Wen Shi
The substrate material is ceramic Al2O3 with a dielectric constant of 9.6 and a thickness of 0.254 mm.
Acknowledgements This material is based upon work funded by Zhejiang Provincial Natural Science Foundation of China under Grant (No.
Liu: Microelectronics Journal Vol. 43 (2012), p. 569 [2] Liu Dan, Wang Liang, Chen Xiaojuan: Microwave and Millimeter Wave Circuits and System Technology: (2012), P. 1 [3]Chen Chi, Hao Yue, Feng Hui, Gu Wenping, Li ZhiMING, Hu Shigang, and Ma Teng: Journal of Semiconductors Vol. 43 (2012), p. 13 [4] Information on http://www.triquint.com/products/p/TGF2023-02 [5] H.
Acknowledgements This material is based upon work funded by Zhejiang Provincial Natural Science Foundation of China under Grant (No.
Liu: Microelectronics Journal Vol. 43 (2012), p. 569 [2] Liu Dan, Wang Liang, Chen Xiaojuan: Microwave and Millimeter Wave Circuits and System Technology: (2012), P. 1 [3]Chen Chi, Hao Yue, Feng Hui, Gu Wenping, Li ZhiMING, Hu Shigang, and Ma Teng: Journal of Semiconductors Vol. 43 (2012), p. 13 [4] Information on http://www.triquint.com/products/p/TGF2023-02 [5] H.
Online since: November 2010
Authors: Chao Cheng Chang
Influences of Strain Rate on Copper Nanowire in Tension
Chao-Cheng Chang
Department of Mold and Die Engineering, National Kaohsiung University of Applied Sciences,
No. 415, Chien-Kung Rd., Sanmin District, Kaohsiung 807, Taiwan
ccchang@cc.kuas.edu.tw
Keywords: Molecular Dynamics Simulation, Strain Rate, Nanowire
Abstract.
This EAM model describes the electron density ( )f r in an exponential form as ( ) exp[ ( )] e e f r f r rχ= − − (3) where ef is a scaling constant and can be taken as 1 for pure materials, er is the equilibrium nearest distance, and χ is an adjustable parameter that must be determined.
Zhang: Journal of Applied Physics Vol. 90 (2001), p. 3090 [2] R.
Raff: Proceedings of the Institution of Mechanical Engineers, Part B: Journal of Engineering Manufacture Vol. 215 (2001), p. 1639 [3] Y.
This EAM model describes the electron density ( )f r in an exponential form as ( ) exp[ ( )] e e f r f r rχ= − − (3) where ef is a scaling constant and can be taken as 1 for pure materials, er is the equilibrium nearest distance, and χ is an adjustable parameter that must be determined.
Zhang: Journal of Applied Physics Vol. 90 (2001), p. 3090 [2] R.
Raff: Proceedings of the Institution of Mechanical Engineers, Part B: Journal of Engineering Manufacture Vol. 215 (2001), p. 1639 [3] Y.
The Research of Calculation Method on Vertical Natural Frequency of the New Full-Prefabricated Floor
Online since: July 2016
Authors: Chong Fang Sun, Xiao Jun Zhu, Shu Ting Liang
Introduction
With the further improvements of structural analysis and construction technologies and the widespread applications of newly lightweight and high strength materials, long-span, flexible and low-damping structures prevail, but the structures have low natural frequency and prominent comfort problems under human-induced loads.
Journal of Performance of Constructed Facilities, 24(6), 508-518
Journal of Vibration and Shock, 31(1), 178-181
Bei Jing: Science press.
Journal of Performance of Constructed Facilities, 24(6), 508-518
Journal of Vibration and Shock, 31(1), 178-181
Bei Jing: Science press.
Online since: December 2012
Authors: Yun Lei Fan, Guo Jing He, Xi Bing Hu, Peng Zhou, Yu Wei Yang
(4) The effects of material nonlinearity and geometrical nonlinearity are not considered
Fig.4 Simplified outline The structure shown above is a eight-story construction, in which the cross-section specification are HN350×175×7×11 and HM390×300×10×16 for columns and beams, respectively, steel elasticity module is E=2.06×105Mpa, as the material is Q235-B, and the connections of beam-column are rigid.The story model provided in this paper, the Smith-Coull Method, the Amendatory Contra-flexure Point Method, and SEASF Program Method[5] are used to calculate the story horizontal displacements of the structure shown in Fig.4.
Acknowledgements This work was financially supported by Hunan Provincial Department of Housing and Urban and Rural Construction Science Foundation (200919), Hunan Provincial Department of Education (Young Teachers’ Project), Youth Foundation of Central South University of Forestry and Technology (2008009A) and the Talent Introduction Foundation of Central South University of Forestry and Technology (104-0054).
Journal of Constructional Research,1999,51(1):37-59 [2] E.M.
Engineering Structures, 1997,19 (8):644-654 [3] Sheng Hongyu.On the solutions of free vibration problem for thick laminated plates by using static elimination method [J].Journal of Hefei University of Technology, 2000,23(6):1019-1022 [4] Hu Xibing.
Fig.4 Simplified outline The structure shown above is a eight-story construction, in which the cross-section specification are HN350×175×7×11 and HM390×300×10×16 for columns and beams, respectively, steel elasticity module is E=2.06×105Mpa, as the material is Q235-B, and the connections of beam-column are rigid.The story model provided in this paper, the Smith-Coull Method, the Amendatory Contra-flexure Point Method, and SEASF Program Method[5] are used to calculate the story horizontal displacements of the structure shown in Fig.4.
Acknowledgements This work was financially supported by Hunan Provincial Department of Housing and Urban and Rural Construction Science Foundation (200919), Hunan Provincial Department of Education (Young Teachers’ Project), Youth Foundation of Central South University of Forestry and Technology (2008009A) and the Talent Introduction Foundation of Central South University of Forestry and Technology (104-0054).
Journal of Constructional Research,1999,51(1):37-59 [2] E.M.
Engineering Structures, 1997,19 (8):644-654 [3] Sheng Hongyu.On the solutions of free vibration problem for thick laminated plates by using static elimination method [J].Journal of Hefei University of Technology, 2000,23(6):1019-1022 [4] Hu Xibing.
Online since: June 2013
Authors: Qin Yang, Hui Liang Zhao, Ai Zheng Yan, Guan Hao Zhao, Sheng Zhao Luo
XING: Journal of Jiamusi University (Natural Science Edition) ,Vol.30 (2012) No.3, p.331
OUYANG: Journal of Automotive Safety and Energy, Vol.3 (2012) No.1, p.44 [9] M.
WANG: Advanced Materials Industry, (2008) No.12, P.16
OUYANG: Journal of Automotive Safety and Energy, Vol.3 (2012) No.1, p.44 [9] M.
WANG: Advanced Materials Industry, (2008) No.12, P.16
Online since: July 2016
Authors: Scott William Sloan, Majidreza Nazem, Nadia Zakrzewski, Mark Cassidy
On Application of the Maximum Entropy Meshless Method for Large Deformation Analysis of Geotechnical Problems
Nadia Zakrzewski1, a *, Majid Nazem1, b, Scott Sloan1, c and Mark Cassidy2, d
Australian Research Council Centre of Excellence for Geotechnical Science and Engineering
1The University of Newcastle, Callaghan NSW 2308, Australia
2The University of Western Australia, Crawley WA 6009, Australia
anadia.zakrzewski@uon.edu.au, bmajidreza.nazem@newcastle.edu.au,
cscott.sloan@newcastle.edu.au, dmark.cassidy@uwa.edu.au
Keywords: Large deformation, Updated Lagrangian, Maximum Entropy Meshless Method
Abstract.
Complexities arise from material nonlinearity, changing boundary conditions, extremely large deformations occurring in the soil, the presence of pore water pressures and, in some cases, dynamic loading.
A static displacement analysis was performed and the behaviour of the clay layer was modelled using the Tresca material model.
Gu, Element Free Galerkin Methods, International Journal for Numerical Methods in Engineering, 37(1994) 229-256
Wright, Overview and construction of mesh free basis functions: From moving least squares to entropy approximants, International Journal for Numerical Methods in Engineering, 70(2007) 181-205
Complexities arise from material nonlinearity, changing boundary conditions, extremely large deformations occurring in the soil, the presence of pore water pressures and, in some cases, dynamic loading.
A static displacement analysis was performed and the behaviour of the clay layer was modelled using the Tresca material model.
Gu, Element Free Galerkin Methods, International Journal for Numerical Methods in Engineering, 37(1994) 229-256
Wright, Overview and construction of mesh free basis functions: From moving least squares to entropy approximants, International Journal for Numerical Methods in Engineering, 70(2007) 181-205