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Online since: July 2011
Authors: Yi Ren Yang, Chen Guang Fan, Ming Lu Zhang, Li Lu
Figure 1.
Figure 3 shows streamlined diagram on the y=1.7m section with two methods.
References [1] E.
Ha: AIAA Journal, Vol. 36 (1998), No.3, P. 477-479
Ma: Journal of Beijing Jiaotong University, Vol. 34 (2010) No.1, P. 14-19.
Online since: December 2016
Authors: Bradley D. Huddleston, Doyl E. Dickel, Neil Williams, Kent Danielson, Mark F. Horstemeyer, Youssef Hammi
Starkville, MS, 39759 U.S.A. 2Bagley College of Engineering, 479-2 Hardy Rd., Mississippi State, MS, 39762 U.S.A. 3ERDC, 3909 Halls Ferry Rd., Vicksburg, MS, 39180 U.S.A.
Figure 1.
At strain rates much higher than 3E+10 s-1, “fragments” do form, though they are clumps of only a few atoms.
References [1] Mott, N.
Phys. 117.1 (1995): 1–19
Online since: February 2014
Authors: Martin Lopušniak
Fig. 1 Typical floor plan and the staircase position Evacuation scenarios.
It is based purely on literature values [1,2,3].
References [1] J.
DiNenno (Eds), SFPE Handbook of Fire Protection Engineering, second ed., NFPA, Quincy, 1995 pp. 1-241 – 1-262
Moss, Simulation of Visibility in Smoke Laden Environments, in: InterFlame 2007, IFSA, London, 2007, pp. 479-491
Online since: January 2013
Authors: Teng Yong Ng, William Toh, Zi Shun Liu
Early studies on the mechanics of gel swelling by Tanaka et al [1] consists of decomposing the material into the two individual phases for separate analysis, which limits the analysis of such materials to simple geometries[1], [2].
The transient process of a cube swelling at various normalized times is shown in Fig. 1.
References [1] Y.
Zhang, “Modeling and simulation of buckling of polymeric membrane thin film gel,” Computational Materials Science, vol. 49, no. 1, pp.
Yang, “pH-Sensitive Hydrogel for Micro-Fluidic Valve,” Journal of Functional Biomaterials, vol. 3, no. 3, pp. 464–479, Jul. 2012.
Online since: April 2007
Authors: Yong Huang, Chun Qing Peng, Chang An Wang, Yang Song
Results and Discussion Fig.1 show the XRD patterns of 20vol%-Cu/Ti3AlC2 synthesized from 850°C to 1100°C and of the Fig.1 XRD patterns of Cu/Ti3AlC2 composite synthesized at different temperature ranging from 850°C to 1100°C.
Therefore, according to the XRD patterns, the reaction between Ti3AlC2 and Cu can be simply illustrated as follows: 3 2 9 4 Ti AlC + Cu TiC + Cu Al → (1) According to the Fig.3 (c), the layered grain in Fig.3 (a) is Ti3AlC2, which has been mentioned in our previous work [9].
References [1] M.
Forum Vol. 475-479 (1-5) (2005), pp. 1247
Vol. 95(1) (2004), pp. 50
Online since: June 2011
Authors: Bo Yang, Xu Lu, Shou Rong Wang, Hong Sheng Li, Li Bin Huang
Besides, if ambient temperature increases from -40ºC to 80ºC, heating power consumption is degraded from 1.27625W to 0.09712W.
(1)
References [1] F.
Li, “Research on Thermal Characteristic in Slow-Small Temperature Changing for MEMS Linear Vibration Gyroscope,” Proceedings of the 2006 IEEE International Conference on Mechatronics and Automation, June 2006, P. 475-479
Chen, Engineering Heat Transfer, Beijing, China: Electric Power Press, 2005,P.1-5.
Online since: July 2012
Authors: Yi He Li, Xiao Dong Li, Jian Feng, Hua Xiao, Gong Yi Li
Introduction Microfluidics for microreactors or chips has attracted great attentions in the past decades [1-3].
After then, the SiC substrate was kept in a 90 ˚C oven for one hour before used. 2.2 Fabrication of microchannels Figure 1.
Laser (b) (c) (a) The experimental process is shown in Figure 1.
References [1] T.
Journal of the Ceramic Society of Japan, 2006, 114 (6): 473-479
Online since: March 2010
Authors: Xin Min Fan, Fei Yan Liu, Jie Wen Huang
The cross-sectional OM microstructute of the specimen treated by HRWD for 4min at a rotating speed of 6500-7200 r/min is shown in Fig. 1.
It also could be seen from Fig. 1 that the near-surface microstructure has been modified greatly after the treatment, the plastic deformation on the surface are produced and plastic flows in the deformation region are found.
Fig. 1 The cross-sectional OM image of the sample HRWD-treated for 4min at a rotating speed of 6500-7200 r/min Fig. 2 is the TEM bright-field image, dark-field image and the corresponding selected area electron diffraction (SAED) pattern obtained at the top surface of the low carbon steel specimen HRWD-treated for 4min at a rotating speed of 6500-7200 r/min.
Fig. 4 TEM bright-field image (a) and dark-field image (b); corresponding SAED (c); histogram of grain size distribution (d) References [1] K.
Forum Vol. 475-479 (2005), p. 133 [7] F.Y.
Online since: October 2007
Authors: Xiao Gang Sun, Chao Ying Xie
Introduction NiMnGa ferromagnetic shape memory alloys (FSMAs) have attracted more attentions for their high up to 6%-10% field-induced strain which is due to magnetically induced twin boundary motion in the martensitic phase [1,2].
Results and discussion Figure 1 shows DSC curves of solution-treated Ni53Mn23.5Ga23.5 particles phase transformation temperatures which were determined as austenite transformation start temperature, i.e.
The storage modulus of Fig. 1 DSC curve of NiMnGa particles Fig. 2 XRD profile of NiMnGa particles Fig. 3 DMA of pure epoxy Fig.4 DMA of NiMnGa composites NiMnGa/polymer composites decreased with temperature more and more quickly than that of pure epoxy.
References [1] S.
Forum Vol. 475-479 (2005), p.2067 [8] R.
Online since: June 2009
Authors: Ren Ke Kang, Han Huang, Zhi Gang Dong
Fig.1.
So the new pile-up occurred only at side "1" of the impression.
At the third stage, cracks started to initiate at the side "1".
References [1] W.C.
A Vol. 479(2008), p. 373 [5] R.
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