Search results

Theoretical calculations of angles are given in table 1.
Table 1 – Theoretical angles of the spring 1008 AISI 304 619A γ 30 α 1°17' 1°26' 1°54' δ 28°43' 28°34' 28°06' Having stamped the part in the die with an elastic element, the following values of angles δ' in table 2 are obtained.
References [1] Rudman L.I.
Metal Science and Heat Treatment, 58(1), 46-50. doi:10.1007/s11041-016-9963-1 [19] Velichko, O.
Metal Science and Heat Treatment, 58(7-8), 479-482. doi:10.1007/s11041-016-0039-z [24] Kolbasnikov, N.

Results and discussion Fig.1 shows the typical hysteresis loop area as a function of temperature for the multilayers with LN=1, 3, 5, 7 and 3D bulk, with τ=19200, H0=4.8, K=1.0, respectively.
The linear variation of Ln(A-A0) versus Ln(1/T ) yields the different scaling exponents γ for the multilayers with LN=1, 3, 5, 7 and 3D bulk.
Especially, for LN≤ 5, the values of α, β and γ change evidently with increasing magnitude of LN, which means 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 0 2 4 6 8 10 12 14 16 18 A T LN=1 LN=3 LN=5 LN=7 PB Fig.1 The typical loop area A as a function of temperature for the multilayers with LN=1, 3, 5, 7 and 3D bulk, with τ=19200, H0=4.8
References [1] B.K.Chakrabarti and M.Acharyya: Rev.Mod.Phys., Vol.71(1998), P.847
[13] Heng Lai, Zhigao Huang et al.: Materials Science Forum Vols. 475-479 (2005), p. 2263 [14] K.

%O and 1.51wt.
References [1] H.
Looney: Key Engineering Matrials Vols. 127-131 (1997) pp 479-486
Hlavacek: Combustion Science and Technology, Vol. 99(1) (1994), pp 161 - 177
Hlavacek: Combustion Science and Technology, Vol. 99(1) (1994), pp 143 - 160.

Table 1.
Fig.1.
Criteria D YM H FT TS TC TEC D 1 0.5 0.333 0.5 0.5 1.610 4.325 YM 2 1 0.5 1.856 1.085 2.726 2.536 H 3 2 1 2.321 1.303 2.189 6.427 FT 2 0.538 0.430 1 1 2 3 TS 2 0.921 0.767 1 1 3 2 TC 0.62 0.366 0.456 0.5 0.333 1 2 TEC 0.231 0.394 0.155 0.333 0.5 0.5 1 Table 5.
References [1] Maity S R, Chatterjee P, Chakraborty S.
Materials & Design, 2013, 45: 473-479

(1) In Eq. (1), CZn and CAl are the concentrations of the respective elements expressed in atomic percentage (at. %).
According to Eq. (1), there is a 0.4 Zn at. % difference from Slice 1 to Slice 6.
Table 1 shows the average values obtained from these results.
References [1] G.
Res. 479-481 (2012) 1303-1306 [4] Q.

Fig.1 Specimen geometry used with the TMF machine Experimental Results.
References [1] J.L.
Stein: International Journal of Plasticity ,Vol. 12 (1996), No.4, pp.451-479
Hyde: High Temperature Technology ,Vol. 4 (1986), No.1, pp.25-29
Hyde: Materials at High Temperatures, Vol. 14 (1997),No.1,pp.27-35.

The FTIR spectrum of chitosan shows the bending vibration of –NH at 1634 cm-1 and the stretching vibration of C-O at 1124 and 1013 cm-1.
References [1] N.
Res., 1 (2012) 43-50
Polym. 63(1) (2006) 61-71
Technol. 40 (2007) 472–479

The parameters are put in table 1.
The schematic diagram is shown in fig.1.
References [1] Raju V R, Kuhn U, Wolff U, et al.
Advances in Mechanics, 1998, 28(4): 479-487.
Acta Armamentarii, 2010, 31(1): 168-171.

Figure 1.
The methane recovery and productivity are 99.5% and 27.6 mmol·kg-1·h-1, respectively.
At this condition, the methane concentration in product gas was enriched to 1.5 vol.% with a methane recovery of 96.3 % and productivity of 41.9 mmol·kg-1·h-1.
Table 1.
Vol. 479-481(2012), p. 648.

Focusing lens, galvanometer 1 rotated around Z-axis, galvanometer 2 rotated around Y-axis are its main components.
Then set A, C axis intersection point O as the coordinate origin, and the coordinates as shown in Fig. 1.
The total transformation matrix from workpiece coordinate system to laser scanner coordinate system is shown as Eq. 1: (1) From the Eq. 1 to reverse its inverse solution, the answer by the following Eq. 2: (2) Kinematic analysis of galvanometric scanning system.
References [1] K.
[2] Yong Zhuo, Yanjun Wu, Juan Peng: Design and Simulation of 3D Layout for MID Based On Open CASCADE, Advanced Materials Research, Vol. 479-481 (2012), pp. 1978-1981