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Lara 1, D.
Prado 1,2 1 CTM-Centre Tecnològic, Av.
Fig. 1.
Table 1.
DC03 1.5mm 0,0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 0,8 -0,4 -0,3 -0,2 -0,1 0,0 0,1 0,2 0,3 0,4 0,5 0,6 ε 2 ε 1 MARCINIAK NAKAJIMA TRIP800 2.0mm 0,0 0,1 0,2 0,3 0,4 0,5 -0,3 -0,2 -0,1 0,0 0,1 0,2 0,3 0,4 ε 2 ε 1 MARCINIAK NAKAJIMA Fig. 8.

Table 1.
Fig. 1.
All spectra confirm CA presence with three main peaks: C=O absorption (1730-1760 cm-1), C−O bond stretching (1210-1270 cm-1), and C−O−C bands (1125-1162 cm-1) [11].
References [1] L.
Sci., vol. 344, no. 1, p. 012040, Oct. 2019, doi: 10.1088/1755-1315/344/1/012040

Fig.1 Models showing possible configurations of VSi –related defects in 6H-SiC lattice in (110) plane.
After optical pumping the rate of the transition from the MS=±1 (MS =±3/2) of the exited state 3E (4E) to the metastable 1E (2E) state is again much larger than the rates of the transitions from the MS=0 (MS=±1/2) sublevel, the rates between the state 1E (2E) and sublevel MS=0 (MS=±1/2) of the 3A (4A) ground state is much less however than the rates of the transitions from 1E(2E) to the levels Ms=±1 (MS=±3/2).
As a result, the spin sublevel MS=±1 (±3/2) of the 3A (4A) ground state is predominantly populated.
References [1] A.
Koehl et al., Nature 479, 84 (2011)

Ti, Nb, V, C, N) [1,2,3].
Fig. 1 - Layout of AST line.
All the significant results of the tensile tests were averaged with Eq.1: ( ) 4 XX2X X 90 45 0 ++ = . (1) where X is any tensile property (i.e.
Table 1 - Chemical composition (% Wt) of studied steels.
References [1] T.

(a) Figure 1: Representation of roughing plunge KO, J.H. (2006) In Fig. 1 (a) illustrates the total contact between tool is part for making a cavity, Fig. 1 (b) represents a process of enlarging a hole through roughing plunge and Fig. 1 (c) shows the machining of a region with partial engagement of the tool at the material.
Table 1: Cutting parameters in plunge milling.
Level Case 1 Case 2 Case 3 Case 4 Case 5 Case 6 Case 7 Case 8 Case 9 rt [mm] 1 1 1 2 2 2 4 4 4 P [mm] 5 6 7,3 5 6 7,3 5 6 7,3 n [RPM] 1989 Vf [mm/min] 318 fz [mm/tooth] 0,08 Vc [m/min] 125 Tool End mill cutter – 20mm with 2 cutting edge (Seco: R 217.79-1620.3-09A) hm calculated[mm] 0,038 0,042 0,05 0,038 0,042 0,05 0,038 0,042 0,05 Cutting parameters Case 1 Case 2 Case 3 rt [mm] 1 2 4 P [mm] 5 6 7,33 VC [m/min] 125 fz [mm/tooth] 0,08 The Table 2 shows the selected cases to evaluate the geometric error in the plunge milling.
The main features are 9 kW power, 7500 rpm maximum spindle rotation and 24 m·min-1 maximum feed speed.
REFERENCES [1] I.

Hastuti 1,b, J.
It can be concluded that : 1.
References [1] S.
Struct. 19 (2010) 1–9
Savvinov, Proc.of ICOMAT-79 (1979) 474-479

Fig. 1: Schematic diagram of the experiment setup Fig. 2: Assembly of the laser rangefinder: 1.
The geometry of the plane-flow hopper can be changed as illustrated in Fig. 1.
The experimental data in Tab. 1 proves, that angle η varies significantly over the different cut-planes examined and is much smaller than the theoretical value of 40°, calculated by Eq. 1.
References [1] Walker, D.M., An Approximate Theory for Pressure and Arching in Hoppers, Chem.
[7] Berry, R.J., Arching Behavior of Cohesive Powder in a Pilot-Scale Plane-Flow Silo, Task Quarterly, (2003) 479-498

The hydrogen bonding condition in a-Si thin films was studied by Fourier transform infrared spectroscope (FTIR, Thermo Nicolet 6700) in the spectral range between 400 and 4000 cm−1 with a resolution of 1 cm−1.
The microstructure factor (R*) of a-Si:H thin films is calculated from the following equation (1) [7, 8, 16]: (1) where I2000 and I2090 are the integrated intensities of FTIR peak at 2000 cm−1 and 2090 cm−1, respectively.
It was observed that all the thin film were amorphous, and the Raman spectrum can be devonvoluted into four parts: the transverse acoustical (TA) mode at 180 cm-1, the longitudinal acoustical (LA) mode at 300 cm-1, the longitudinal optical (LO) mode at 410 cm-1 and the transverse optical (TO) mode at 480 cm-1.
The ωTO, ГTO, ITA/ITO and ILA/ITO of the a-Si thin films with H-ion gases were 479 cm−1, 62 cm−1, 0.38 and 0.27, respectively, which was comparable with that of the plasma deposited a-Si:H thin films [17].
References [1] J.

Rahman 1,f, F.
The proton conductivity of Nafion 117 is 22.23 x 10-3 S cm-1 while the proton conductivity of pristine SPEEK is 6.99 x 10-3 S cm-1.
References [1] J.
May, pp. 1–8, 2016
Sci., vol. 479, pp. 46–54, 2015.

Introduction On account of their excellent combination of mechanical properties at elevated and high temperatures, nickel-based superalloys play a key role in many industrial applications [1].
Fig. 1.
Generally, diffusion rates for FCC metals such as Ni are low[1].Therefore, considerable microstructural stability could be imparted at elevated temperatures.
References [1] R.C.
Charact. 144 (2018) 479-489