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Fig.1.
It is noted that, since Eq.(1) involves the work functions W1 and W2 of metals with free and clean surfaces.
Results and discussions The out-of-plane polarization P-E loops [8] of (001) -oriented ultrathin films for nanoscale (10 nm, 20nm, 50nm) capacitors were simulated under different values of interfacial capacitances ci, equals to (1/cm1 + 1/cm2)-1, to verify the validity of the model, as shown in Fig. 2.
References [1] F.
[19] Values of the materials parameters (in SI units, where the temperature T in ℃) used in the simulation. α1=3.8(T-479)×105, α11=-2.097×108, α111=1.294×109, α123=-2.5×109, α1111=3.863× 1010, Q11=0.1, Q12=-0.034, Q44=0.058, c11=1.78×1011, c12=0.96×1011, c44=1.22×1011, G11=2.786 ×10-10

Fig.1 is the CCT continuous cooling transformation curve diagram for carbon steel bar with the same diameters by taking the temperature as Y-coordinate and the diameter of the time as X-coordinate, from which transformation of the structures when carbon steel bar with the same diameters is cooled by the different cooling rate can be read out. [1,2] 1.2 CCT curves and establishment of the dynamic phase diagram Fig.1.
Take Fig.1 as an example.
The visualized output of the phase diagram are shown as follows: if((pDoc->m_Graphics.m_FeCPhaseArray[j].xArray.GetSize()<1) || (pDoc->m_Graphics.m_FeCPhaseArray[j].yArray.GetSize()<1)) continue; // to judge the array is not empty; nCount =pDoc->m_Graphics.m_FeCPhaseArray[j].yArray.GetSize();// calculate the value of the array //obtain the data at the first point x = pDoc->m_Graphics.m_FeCPhaseArray[j].xArray.GetAt(0); y = pDoc->m_Graphics.m_FeCPhaseArray[j].yArray.GetAt(0); // obtain the data at the first point // scaling, conversion of coordinates,; move to the first point; pDC->MoveTo(c2v(x*pDoc->m_dContentAxisScale, y*pDoc->m_dTmpAxisScale)); …………..
Reference [1] Zou, Q.; Cao, H.; Wang, Z.; Zhang, Z.; Chen, X., Dynamic phase diagrams and non-equilibrium lever principle of carbon steel[J].Materials Technology, 2006，21(1)：21-27
[2] Z Qing-Hua, C Hong, C Xiao-Dao, New-Type Dynamical Phase Diagrams and a Nonequilibrium-Lever Rule for Carbon Steels[J].The Physics of Metals and Metallography, 2005，100 (5)：472-479

Kinematic models Fig. 1.
Also, in Fig. 1 the coordonate conversion operators are depicted.
Now we have all the components in order to determine the operator from relation (1).
REFERENCES [1] D.
Control, vol. 17, 3 (1973) 471-479

(1) (In the expression, subscript 1 denotes fractured medium, subscript 2 denotes matrix rock medium.)
References [1] LI Shun-chu and HUANG Bing-guang.
Well Testing, 2002.11(5):1~3
Application Mathematics and Mechanics, 2004,25(1):93~99
Journal of Oil, 2011, 32(3):479~483

Table 1.
Fig.1 (b) and (c) present the calculated energy band structures of Zn0.875M0.125O (M=Fe, Co).
Fig. 1 Band structures: (a) Pure ZnO, (b) Fe doped ZnO, (c) Co doped ZnO.
This result somewhat agrees well with the reported theoretical result by Gao X.Q. et al. [1].
Li, et al., Chemical states of gold doped in ZnO films and its effect on electrical and optical properties, Journal of Alloys and Compounds, 585 (2014) 479-484

Error analysis is displayed in Table 1.
References [1] Lin Haixue.
Power System Technology, 2003, 27(1): 65-70.
Proceedings of the CSEE, 2007, 27(1): 93-97.
Applied probability and statistics, 2010, 26(5):477-479.

Copper, iron, stainless steel, or other piping materials may be used to carry the cooling medium [1].
The numerical results obtained are summarized in Tables 1 and 2.
Table 1.
Energy-economical criterion c Econ. crit. y = 0 y = 0.25 y = 0.50 y = 0.75 y = 1.00 EP MW EP MW EP MW EP MW EP MW EP MW 0 1 2 3 4 5 6 7 8 9 10 11 12 0.060 236 334 407 697 351 554 315 479 289 429 270 394 0.065 356 561 323 488 299 444 281 411 0.070 361 568 330 500 309 458 294 428 0.075 365 575 338 511 319 473 306 445 Table 2.
*Corresponding Author Ioan Sarbu, Email: ioan.sarbu@ct.upt.ro, Fax: 0040256403987, Phone: 0040256403991 References [1] R.S.

Interface Microstructure of TiC Cermets/Steel Explosive Cladding Plate Li Yan 1,a, Wei Shi-zhong 1, Gao Jian-ping1, Zhang Wan-hong2and Long Rui2 1 Mat.
Fig. 1 (b) is the image to show this characteristic.
References [1] Y.
Vol. 49[1] (2000), p.5
Vol. 479 (2005), p.3855

Verification of process fluids in mass production Jozef Zajac 1, a, Dušan Mitaľ1,b and Peter Michalik 1,c 1 Faculty of Manufacturing Technologies Technical University in Košice with seat in Prešov, Štúrová 31, Prešov 080 01 Slovakia ajozef.zajac@tuke.sk ,b dusan.mital@tuke.sk ,cpeter.michalik@tuke.sk Keywords: processing fluids, forming, monitoring and diagnostic of processing fluids Abstract.
Radial component is 1, 3 times smaller than tangential in the process of dry grinding.
Diagrams are on figures 1 to 4.
Strojírenská technológie V. č.1., str. 10-16, ISSN 1211-4162
Transfér 2005, str.479-484, ISB N80-8075-070-X

Results Creative performance The results showed that our sample obtained high mean scores in fluency (M=10,96, sd=1,5) and flexibility (M=7,75, sd=1,4), scores below the average in elaboration (M=9,75, sd=4,3) and in production of titles (M=13,79, sd=3,6), scores around the average in originality (M=22,94, sd=4,8).
In general, pupils obtained average scores in total creative performance below standard average (M=65,19, sd=11,1).
Curiosity was positively correlated with complexity (r=.530, p<.001), imagination (r=.507, p<.001), and willingness to take risks (r=.461, p<.001).
Complexity was positively correlated with imagination (r=.479, p=.001) and willingness to take risks (r=.531, p<.001).
References [1] J.P.