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Compared with graphite (372mAh∙g-1), the silicon-based anode materials has an extremely high theoretical specific capacity (4200mAh∙g-1 and 3580mAh∙g-1) [1].
The reversible capacity of 989.5 mAh∙g-1 at 2.1 A∙g-1 and 345 mAh∙g-1 at 12.6 A∙g-1.
Zhuang et al.[15]prepared Si@porous-C composite materials by using nano-MgO as the pore-former,as shown in Fig.3,Si@porous-C can provide reversible capacities of 947 mAh∙g-1, 670 mAh∙g-1,and 394 mAh∙g-1 at current densities of 1 A∙g-1, 2 A∙g-1, and 4 A∙g-1,respectively.
The SiOx@C composites has high initial coulombic efficiency (75.1%), and with 83% capacity retention rate for 500 cycles at 1 A∙g-1,and 907.7 mAh∙g-1 at 2 A∙g-1.
Applied Surface Science, 2019,479:896-902

A superplastic elongation of 1090% is evident in Fig. 1 at an initial strain rate of 1.0 × 10-2 s-1 where this is within the high strain rate superplasticity regime.
Summary and conclusions 1.
W911NF-05-1-0046.
References [1] T.G.
Forum Vol. 475-479 (2005) p. 2937

Comparison of thermogravimetric curves (Fig. 1 and Table 1) makes it possible to detect obvious differences both between stabilized and non-stabilized PEEK samples, and in the effectiveness of the stabilizers used.
The difference in the concentration dependence of the MFI of the PEEK samples stabilized with Ethaphos 368 is that first there is an increase in the viscosity of the melt to 1-1.25% of the stabilizer content; stabilizer.
It also lists the properties of PEEK stabilized with 1% Hostanox “P-EPQ.
Efficiency and mechanism of phosphorous antioxidants in Phillips type polyethylene, Polymer degradation and stability 91, 3 (2006) 479 [13] Zhou Zheng, Zhou Fu-gui, Zhang Shu-ling, Mu Jian-xin, Yue Xi-gui and Wang Gui-bin.
Chinese Universities. 21-1 (2005) 109

The observations in Fig. 1(b) are generally similar to Fig. 1(a) with similar conclusions.
References [1] R.T.
Ahmad, Selection of materials for corrosive environment, Principles of Corrosion Engineering and Corrosion Control Chapter 9, 2006, pp. 479-549
Sci. 7(1) (2012) 9423-9440 [19] R.
URSS 1 (1934) 961–973.

The atmosphere was dry industrial air with a flux of 1.5lr/hr.
Fig. 1 shows the structure of three as cast Cr-Ni-Al alloys.
(a) Cr-5-5 (b) Cr-5-10 (c) Cr-10-10 Fig. 1.
Calculated NiAl-Cr diagram according to Dupin et al. [9] Sample Cr Ni Al Cr-5-5 91,4 ± 1,7 4,2 ± 1,1 4,4 ± 0,6 Cr-5-10 87,1 ± 1,2 3,9 ± 0,7 9,0 ± 0,5 Cr-5-15 80,9 ± 0,9 4,1 ± 0,4 15,0 ± 0,5 Cr-8-8 91,8 ± 0,9 3,1 ± 0,5 5,1 ± 0,4 Cr-10-10 89,8 ± 0,6 4,1 ± 0,4 6,1 ± 0,2 As-cast alloys are not at thermodynamic equilibrium: nevertheless, these observations are in relatively good agreement with the NiAl-Cr phase diagram (Fig. 2) provided by Dupin et al. [6] which states the maximum solubility of NiAl in chromia to 14at%.
-10.0 -7.5 -5.0 -2.5 0.0 2.5 5.0 7.5 Onset point : 1 435,05 °C Peak 1 top : 1 446,88 °C 1431°C 1404°C Heat Flow/ µV Temperature/ °C 1250 1300 1350 1400 1450 -10.0 -7.5 -5.0 -2.5 0.0 2.5 5.0 7.5 Onset point : 1 435,05 °C Peak 1 top : 1 446,88 °C 1431°C 1404°C Heat Flow/ µV Temperature/ °C 1250 1300 1350 1400 1450 Fig. 3.

Valiev 1,a,* , Maxim Yu.
Fig. 1.
Mechanical properties of 6061 alloy after ECAP-PC through 1, 2 and 4 passes are presented in Fig. 5 and Table 1.
References [1] R.Z.
Vols. 475-479 (2005), p. 3131 [34] B.B.

Table 1.
Figure 1.
Acknowledgements This research was funded by European Regional Development Fund (ERDF) and Latvian State, Project agreement No. 1.1.1.2/16/I/001, research application No. 1.1.1.2/VIAA/1/16/186.
Cregg et al., High-level expression and efficient assembly of hepatitis B surface antigen in the methylotrophic yeast, Pichia pastoris, Bio/Technology. 5:5 (1987) 479–485
J. 30:1 (2016)

A lower deviation of 1 is desirable.
AC 2.78 1 2.78 10.49 0.0230 Sign.
Manuf. 1(2014)99-109
Sci. 126(2017)479-490
Process. 1(2019)

Ak and Bk have been determined by applying the continuity equations for potential and its derivative at respective boundaries given as below: and where, i = 1, 2.....7 and k = 1, 2...7 and .
Table 1 Static performance parameters for p-n-i-n H-D TFET with varying LHfO2.
Vds = 1.0V and φm = 4.0 eV.
References [1] D.
Riel, Tunnel field-effect transistors as energy-efficient electronic switches, Nature. 479 (2011) 329-337

Fig. 1.
Table 1.
References [1] D.
Eng., (2013), pp. 1–9 [19] L.
Soc., vol. 85, no. 4, (1963), pp. 478–479