Search results

Fig. 2a&b X-ray diffraction patterns of Pristine and 10 at.% In-doped ZrO2 thin films Fig. 3aDecreasing the plane (111) intensity, 3b Increasing the plane (200), (220) and (311) intensities of Pristine ZrO2 thin film Moreover, the desired peaks were observed from the Bragg angles 2θ at 30.19o, 35.33o, 50.54o, and 60.13o strongly possessed with the preferred miller planes are (1 1 1), (2 0 0), (2 2 0) and (3 1 1), appropriately [14, 15].
Notably, the peak intensity of the Pristine ZrO2 thin film at (1 1 1) plane has slightly decreased with the addition of 10 at.% of Indium, as illustrated in Fig.3a.
The calculated microstrain and dislocation density values are parallel increased 3.79 to 4.34x10-3 and 1.115 to 1.458x1016, are presented in the Table 1.
Ser. 61, 11 (2007). http://dx.doi.org/1 0.1088/1742-6596/61/1/003 [26] Sajid I.
Sreedhara Reddy, J ALLOY COMPD.479, 589 (2009)

The proposed variants are described as follows: Variant 1.
As and are random numbers which belong to the open interval ]0, 1[.
Table 1 Limits of reactive power generation (p.u) for IEEE 14-bus and 30-bus systems 14 -bus 30-bus 57-bus Bus no.
References [1] A.
In 2019 International Conference on Innovative Trends in Computer Engineering (ITCE) (pp. 479-484).

Analysis showed that the pore size was governed by the porogen and not influenced by the SF/PVA ratio (Table 1).
Figure 7: ALP activity assay of hMSCs grown on developed scaffolds for 1 day, 7 days and 14 days.
References [1] R.
Pharmacol., 47 (1995) 479–486
Dev., 1 (2010) 404–408

Contents of Paper 1.
Conclusions References 1.
Fig. 1.
References [1] L.
Meas. 27 (1997) 479-488

Table 1.
(1) Figure 1.
ANOVA outputs of the developed model Source Sum of squares df Mean square F value p-value Model 4.53E+07 14 3.24E+06 13.41 < 0.0001 significant A-A 0 1 0 0 1 B-B 3.69E+06 1 3.69E+06 15.28 0.0014 C-C 1.80E+06 1 1.80E+06 7.44 0.0156 D-D 1.90E+07 1 1.90E+07 78.75 < 0.0001 AB 0 1 0 0 1 AC 0 1 0 0 1 AD 0 1 0 0 1 BC 1.51E+06 1 1.51E+06 6.24 0.0246 BD 1.92E+06 1 1.92E+06 7.94 0.013 CD 1.84E+06 1 1.84E+06 7.62 0.0146 A2 1.69E+05 1 1.69E+05 0.7 0.4164 B2 2.63E+06 1 2.63E+06 10.87 0.0049 C2 2.33E+05 1 2.33E+05 0.97 0.3414 D2 2.67E+06 1 2.67E+06 11.03 0.0047 Residual 3.62E+06 15 2.42E+05 Lack of Fit 3.62E+06 10 3.62E+05 Pure Error 0 5 0 Cor Total 4.90E+07 29 Equation (3) shows the modified model of the relationship between the integral absolute error and the selected tuning parameters of the model predictive control system.
ANOVA outputs of the modified model Source Sum of squares df Mean square F value p-value Model 4.48E+07 9 4.98E+06 23.73 < 0.0001 significant A-A 0 1 0 0 1 B-B 3.69E+06 1 3.69E+06 17.6 0.0004 C-C 1.80E+06 1 1.80E+06 8.57 0.0083 D-D 1.90E+07 1 1.90E+07 90.75 < 0.0001 BC 1.51E+06 1 1.51E+06 7.19 0.0144 BD 1.92E+06 1 1.92E+06 9.14 0.0067 CD 1.84E+06 1 1.84E+06 8.79 0.0077 B2 2.06E+06 1 2.06E+06 9.84 0.0052 D2 2.10E+06 1 2.10E+06 10.03 0.0048 Residual 4.19E+06 20 2.10E+05 Lack of Fit 4.19E+06 15 2.80E+05 Pure Error 0 5 0 Cor Total 4.90E+07 29 The analysis of variance (ANOVA), the results of which is given in Table 6, carried out on the modified model showed each of the factors to have a p-value that was less than 0.05 except that of the factor A, which was not eliminated deliberately so as to have a control horizon as a tuning parameter in the control system.
Hapoglu, Adaptive Neuro-Fuzzy Inference Systems (ANFIS) modeling of reactive distillation process, ARPN Journal of Engineering and Applied Sciences, 8(7) (2013) 473-479

Consequently , in the �ell integration metho d, the domain integral in the equation (1) �an b e expressed as (see Salgado and Aliabadi [13 ℄): 1 hS Z 
 R U �S ij �x0 ; x� bj (x) d
R � = 1 h S n�el l s X k =1 Z 
k U �S ij �x0 ; x � b j ( x) d
 k (5) and the integration is �arried out on ea�h �ell.
In this �ase the integrand in (6) �an b e regularized at the singular p oint by substra�ting suitable singular term, whi�h may b e treated separately as follow (see Y oung and Ro oke [11 ℄): Z 
k U �S ij Nj k d
k = 1 Z �1 �1 Z �1 n U �S ij Nj k J � �ij ln (R ) J o d� d� +�ij J 1 Z �1 �1 Z �1 ln ( R ) d� d� (7)where, R = p(� � � o )2 + (� � �o )2 .
Referen�es [1℄ Rose L.
International Journal of F ra�ture, 3(1): 51-64, (1977)
(eds), 463-479, San Antonio, EUA, (1988)

Figure 1.
Table 1.
The wave numbers at 877, 740, 686.5, and 543 cm-1 were due to aromatic C-H out-of-plane bending [29] and at 792.5 cm-1 is generally assigned to the out-of-plane bending mode of aromatic C-H groups in 1, 4-disubstituted aniline units [19] which indicates the head-to-tail coupling in PANI.
Vegetable oil based eco-friendly coating materials: A review article, Arabian Journal of Chemistry 7(4), pp. 469-479 [14] Jaroslav Stejskal (2002).
Sci Rep. 2019 Nov 6; 9(1) :16081. doi: 10.1038/s41598-019-52635-2.

Table 1.
Step 1.
References [1] R.
Res. 165 (2005) 479–494
Quart. 1 (1954) 61–68

a b c a c b c b a β B2 M-phase Lattice correspondence a0 Fig.1.
(1) under invariant plane strain condition.
Strain (%) Stress (MPa) 0 100 200 0 100 200 1% (a) 823K 0 100 200 300 400 (b) 873K (c) 973K 1% 1% 1st 2nd 3rd 5th 7th 10th 1st 2nd 3rd 5th 7th 10th 1st 2nd 3rd 5th 7th 10th Fig. 20.
References [1] W.
Miyazaki: Materials Science Forum Vol. 475-479 (2005), p.2037 [49] M.

In order to verify this combination of high strength and good ductility, the two loading modes were performed at higher (0.417 s-1 and 4.17s-1) and lower (4.17×10-5 s-1 and 4.17×10-6 s-1) strain rates, respectively.
From the ln−σ curves in the inset of Fig. 8(c), the corresponding average v* values were measured to be 6.3b3 at ≤10-2 s-1 and 8.7b3 at ≥10-2 s-1.
The following conclusions can be drawn: 1.
A Vol. 479 (2008), p. 136
Vol. 1 (2002), p. 45