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In consequence the particle will be carried away (Fig. 1).
Fig. 1: Droplet on a lotus leaf.
References [1] T.
Moilliet (Elsevier, Amsterdam, 1963), pp. 1
Quéré: Nature Materials Vol. 1 (2002), p. 14 [24] W.R.

The construction of ECAP processing is schematically presented in Fig. 1(a) and the determination of longitudinal and cross-sectional planes of the specimen after ECAP processing is depicted in Fig. 1(b).
The XRD equipment used was D5000 Siemens Diffractometer with CuKα radiation (λ=1.5406Å).
Table 1.
References [1] I.
Samuel, Effect of grain refiner on the tensile and impact properties of Al–Si–Mg cast alloys, Materials and Design. 56 (2014) 468-479

In order to conduct nondestructive evaluation of the extent of structural damage, the magnetic Barkhausen noise [1], neutron diffraction [2], and positron annihilation [3] methods were employed.
xkA A 22 1 28 =β (1) where A1 and A2 are the fundamental and second-harmonic frequency amplitude, respectively, x (8mm) is the wave propagation distance and k ( 2π×10MHz) is the wave number.
The change in the ultrasonic velocity was only about 1 %, while the attenuation coefficient increased by several tens of percent.
References [1] V.E.
Forum Vol. 475-479 (2005), p. 4117 [8] M.A.

Methyl fluoride is stable, which is not the compound in 1 or 2 degree of ozone depletion potential.
References [1] R.
Beijing:Chemical Industries Series, 2007, pp.1-79 [4] I.
Marine and Petroleum Geology, vol. 18, Apr. 2001, pp. 479-486 [23] A.
McGrail, “Designing a pilot-scale experiment for the production of natural as hydrates and sequestration of CO2 in class 1 hydrate accumulations”, Energy Procedia, vol.1, Feb. 2009, pp. 3099-3106 [30] G.

The samples of K2Gd1-x-yZr(PO4)3 : Tb3+, Er3+ (0.5 mol. % ≤ x ≤ 5 mol. %, 1 mol. % ≤ y ≤ 5 mol. %) were prepared by solid-state reaction method.
The XRD patterns are shown in Fig. 1.
Figure 6 Excitation Spectra of K2Gd1-x-yZr(PO4)3 : Tb3+, Er3+ (0.5 mol. % ≤ x ≤ 5 mol. %, 1 mol. % ≤ y ≤ 5 mol. %) under UV and VUV Excitation, Monitored at 550 nm.
References [1] Y.
Mater. 32 (2010) 479

Related dimensions are as following: l=37 mm, h=15 mm, r=3.25 mm, 8 mm≤x≤30 mm, 1 mm≤y≤4 mm.
The reference values of material properties, element types are shown in Table 1.
References [1] Zhili Long, Lufan Zhang and Jianguo Zhang: Advanced Materials Research.
Vol. 479-481 (2012),p. 434 [2] George Harman: Wire Bonding in Microelectronics: Materials, Processes, Reliability, and Yield, 2nd ed.
Vol. 1(2011), p. 124

Introduction MEMS accelerometers have the merits of low power consumption, high sensitivity and small size [1].
Let us define the 3-axis accelerometers output , Figure. 1.
and the acceleration vector, which is expressed in the 3-axis accelerometers local referen-ce system (Fig.1). is the true acceleration in each axis.
The ultimately model of 3-axis accelerometers is given by: (1) Where ,.
[9] Qiang Zhao, Yongheng Yue and Qiang Guan, “A PSO-based Ball-plate Calibration for Laser Scanner”, International Conference on Measuring Technology and Mechatronics Automation, Zhangjiajie, China, April 11-12, 2009, pp.479-481

References [1] D.
Failure Analysis and Prevention, 2007, 12(1): 38-42
Materials Science and Engineering A, 2009, 520: 1-10
Oxidation of Metals, 1995, 44(1/2): 3-27
Foundry, 2014, 63(5): 479-483.

Figure 1.
Given a set of control points, Thin-plate-spline function basically defines a spatial mapping which maps point into a new location represented by, (1) where denotes the Euclidean norm and is a set of mapping coefficients.
References [1] G.
In Proceedings of ACM SIGGRAPH 2000, 479–488
Splines minimizing rotation invariant seminorms in sobolev spaces, constructive theory of functions of several variables, 1, pp 85-1

Research on the JWL Parameters of Several Kinds of Explosives Hisaatsu Kato 1,a, Noriyuki Kaga 1,b, Michinori Takizuka 1,c, Hideki Hamashima 2,d, Shigeru Itoh 3,e 1 Nippon Koki Co., Ltd.
Experiment 2-1.
These are shown in Table 1.
5.5355.5355.5355.535 5.5015.5015.5015.501 5.3015.3015.3015.301 1.4791.4791.4791.479 1.4731.4731.4731.473 1.4711.4711.4711.471 1.4671.4671.4671.467 1.4711.4711.4711.471 1.4241.4241.4241.424 1.4251.4251.4251.425 1.3521.3521.3521.352 0.2950.2950.2950.295 0.2900.2900.2900.290 0.2910.2910.2910.291 0.2880.2880.2880.288 0.2920.2920.2920.292 0.2580.2580.2580.258 0.2160.2160.2160.216 0.1740.1740.1740.174 0.0820.0820.0820.082 0.0790.0790.0790.079 0.0800.0800.0800.080 0.0780.0780.0780.078 0.0790.0790.0790.079 0.0570.0570.0570.057 0.0170.0170.0170.017 0.0120.0120.0120.012 Comp.C4Comp.C4Comp.C4Comp.C4 Comp.C4+GMB20% Comp.C4+GMB20% Comp.C4+GMB20% Comp.C4+GMB20% ＥｏＥｏＥｏＥｏ NS- 201NS- 201NS- 201NS- 201 NS- 211NS- 211NS- 211NS- 211 BBBB R1R1R1R1 R2R2R2R2 ωωωω Det.
References [1] M.