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Online since: July 2013
Authors: Xin Wu Huang, Ji Cheng Zhou, Zhi Bai Xie, Jing Jing Liao, Si Wei Liu
The above chemicals were mixed at a predetermined molar ratio of Li:Mn = 1:2, and then in distilled water.
Results and discussion XRD analysis The XRD pattern of the synthesized powders is shown in Fig.1.
Fig.1.
References [1] J.M.
Vol. 479 (2009), p. 310
Results and discussion XRD analysis The XRD pattern of the synthesized powders is shown in Fig.1.
Fig.1.
References [1] J.M.
Vol. 479 (2009), p. 310
Online since: September 2013
Authors: Shou Guang Yao, Gong Li Wang, Qing Fang Cheng, Chang Jiang Zhou
Lattice Boltzmann method for numerical simulation of circular tube forced convection
Shouguang YAO 1, a,Gongli WANG 2, b,Qingfang CHENG 3, c,
Changjiang ZHOU 4
1,2,3,4School of Energy and Power Eng.
This paper established the thermal Lattice Boltzmann model of fluid flow and heat transfer, which is based on double lattice Boltzmann distribution model[1].
(1) In this function, ; is the speed of the particle distribution function; is the speed of the particle equilibrium distribution function accordingly.
References [1] Shen X, Chen H.
Europhysics Lett(1992), 17:479-484 [5] Guo Z L, Zheng C G, LI Q.
This paper established the thermal Lattice Boltzmann model of fluid flow and heat transfer, which is based on double lattice Boltzmann distribution model[1].
(1) In this function, ; is the speed of the particle distribution function; is the speed of the particle equilibrium distribution function accordingly.
References [1] Shen X, Chen H.
Europhysics Lett(1992), 17:479-484 [5] Guo Z L, Zheng C G, LI Q.
Online since: September 2014
Authors: Bang Jun Lv, Jia Chen, Li Kun Peng
The kinematic Jacobian matrix condition number (CDN) was first introduced by Salisbury et al as an optimization indicator for Stanford/JPL robot[1].
References [1] Salisbury J K, Craig J J.
Int J Rob Res, 1982, 1(1): 4-17
Joumal of Robotic Systems, 1993, 10(4): 463-479
J Robotics Syst, 1985, 2(1): 113-124
References [1] Salisbury J K, Craig J J.
Int J Rob Res, 1982, 1(1): 4-17
Joumal of Robotic Systems, 1993, 10(4): 463-479
J Robotics Syst, 1985, 2(1): 113-124
Online since: August 2018
Authors: H.D. Wang, Zhi Qiang Sun, Heng Dong, Yi Lu, Shu Qin Li
To begin of all, tetraethoxysilane and n-octylamine were mixed together (volume ratio 1:1) and stired at 300 r/min for 3 min.
From the magnified SEM image in Fig. 1(b), it is further found that the surface of HSSs is smooth without visible flaws and pores.
Fig. 1 The optical image (a) and SEM image (b) of HSSs.
References [1] J.K.
Sci. 3 (1998) 474-479
From the magnified SEM image in Fig. 1(b), it is further found that the surface of HSSs is smooth without visible flaws and pores.
Fig. 1 The optical image (a) and SEM image (b) of HSSs.
References [1] J.K.
Sci. 3 (1998) 474-479
Online since: April 2009
Authors: Geun Tae Bae, Dong Hyuk Shin, A.K. Prasada Rao, K.H. Kim, J.H. Bae, Nack Kim
Kim
1, J.
Bae 1, G.T.
Bae 1, D.
Figure 1.
[2] Park, S.S., Kim, Y.M., Kang, D.H. and Kim, N.J. (2005) Materials Science Forum 475-479, 457-462
Bae 1, G.T.
Bae 1, D.
Figure 1.
[2] Park, S.S., Kim, Y.M., Kang, D.H. and Kim, N.J. (2005) Materials Science Forum 475-479, 457-462
Online since: May 2013
Authors: Yi Lin Chi, Bin Hua, Yan Fang Ding, Xue Jun Wang
Clamping and squeezing the stone to flow under the sleeper and vibrating compresses ballast [1].The tamping device produced by PLASSER mainly realizes two movements: rocking path and asynchronous clamp, which elevate sleepers to a desire position [2].
Fig.1 shows the structure of the tamping device. 1.Outside tamping tine 2.Inside tamping tine 3.
Table.1 The mechanism parameters of tamping device OA[mm] AB[mm] BC[mm] CD[mm] 2.5 505 390 683 Initial design parameters.
Meanwhile, the max horizontal velocity showing in the fig.7 (a) is about 1 m/s, while the velocity taking on in the fig.7 (b) is about 0.009m/s in the vertical direction.
Vols. 479-481, in 2012, pp 1395-1398
Fig.1 shows the structure of the tamping device. 1.Outside tamping tine 2.Inside tamping tine 3.
Table.1 The mechanism parameters of tamping device OA[mm] AB[mm] BC[mm] CD[mm] 2.5 505 390 683 Initial design parameters.
Meanwhile, the max horizontal velocity showing in the fig.7 (a) is about 1 m/s, while the velocity taking on in the fig.7 (b) is about 0.009m/s in the vertical direction.
Vols. 479-481, in 2012, pp 1395-1398
Online since: May 2019
Authors: Dong Ying Ju, Zhi Pu Pei, Hai Jian Wang
Table 1.
The dimension of the specimen is shown in Fig.1.
Fig.1.
References [1] Xu W, Birbilis N, Sha G, et al.
J Shanghai Jiaotong Univ (Sci), 2012, 17(4): 479-483
The dimension of the specimen is shown in Fig.1.
Fig.1.
References [1] Xu W, Birbilis N, Sha G, et al.
J Shanghai Jiaotong Univ (Sci), 2012, 17(4): 479-483
Online since: February 2012
Authors: Yi Bo Yang, Y. Yu, W.P. Chen
Structure design
The structure of the device is shown in the Fig.1.It is a symmetrical structure which mainly consists of two large proof masses.
The designed dimensions are given in table 1.
Table 1.
Syst. 15 (3) (2006) 479–491 (doi:10.1109/JMEMS.2006.876779) [4] U.
International Solid-State Sensors, Actuators and Microsystems Conference TRANSDUCERS 2005, vol. 1, 2005, pp. 184–187 (doi:10.1109/SENSOR.2005.1496389)
The designed dimensions are given in table 1.
Table 1.
Syst. 15 (3) (2006) 479–491 (doi:10.1109/JMEMS.2006.876779) [4] U.
International Solid-State Sensors, Actuators and Microsystems Conference TRANSDUCERS 2005, vol. 1, 2005, pp. 184–187 (doi:10.1109/SENSOR.2005.1496389)
Online since: September 2023
Authors: Hyo Woon Hwang, Dong Geun Lee
Table 1 presents the relative raw material costs for Ti-xMo-2Fe (x = 3.4 and 9.2 wt%) and other titanium alloys based on the reported metal prices.
Table 1.
Fig. 1.
References [1] M.
Vol. 479 (2009) p. 699-703
Table 1.
Fig. 1.
References [1] M.
Vol. 479 (2009) p. 699-703
Online since: March 2013
Authors: Tobias Binder, Ilka Weikusat, Johannes Freitag, Christoph S. Garbe, Dietmar Wagenbach, Sepp Kipfstuhl
Reflected light imaging of polished surfaces prepared by controlled sublimation etching [1,2] reveals deep grooves along grain boundaries and shallow grooves along sub-grain boundaries (Fig. 1) [3].
An example is shown in Fig. 1.
In the NEEM deep ice core high bubble pressures induced the formation of (sub-) grain boundaries in the vicinity of bubbles because of the high storage temperature (see Fig. 1).
References [1] L.
Glaciol. 53 (2007), 479-489
An example is shown in Fig. 1.
In the NEEM deep ice core high bubble pressures induced the formation of (sub-) grain boundaries in the vicinity of bubbles because of the high storage temperature (see Fig. 1).
References [1] L.
Glaciol. 53 (2007), 479-489