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21 Nov 2014: 1" > </div> <div class="sg" id="s54" data-sgid="Picture 72" style="z-index:25;left:174.76px;top:187.45px;width:15.95px;height:24.81px"> <img class="sg" ... 73AAA3D7.png" id="s54_i" style="z-index:1;left:0px;top:0px;width:15.95px;height:24.81px" > </div>

19 Nov 2014: alt="TP_tmp.png" style="z-index:1;left:0px;top:0px;width:610.48px;height:20.85px" > </div> <div class="sg" id="s30" data-sgid="Picture 24" ... s52_i" title="" alt="TP_tmp.png" style="z-index:1;left:0px;top:0px;width:126.80px;height:20.87px" > </div> <div

18 Nov 2014: width:286.66px;height:31.20px" > </div> <div class="sg" id="s54" data-sgid="Picture 33" ... top:506.17px;width:537.68px;height:24.83px"> <img class="sg" src="5EA7B95C.png" id="s47_i" title="" alt="x3.pdf"

15 Nov 2014: 0px;width:35.72px;height:24.92px" > </div> <div class="sg" id="s43" data-sgid="Picture 72" ... Picture 87" style="z-index:24;left:254.02px;top:367.31px;width:247.82px;height:25.55px"> <img class="sg" src="B1ABE4BD.png" id="s50_i" title=""

15 Nov 2014: 46.76px" > </div> <div class="sg" id="s17" data-sgid="Rectangle 24" style="z-index:5;left:63.46px;top:282.31px;width:638.56px;height:46.88px" data-fillcolor="16777215"> ... width:360.28px;height:28.07px" > </div> <div class="sg" id="s53"

28 Nov 2014: div class="sg" id="s18" data-sgid="Picture 59" style="z-index:6;left:44.62px;top:191.64px;width:24.96px;height:28.30px"> <img class="sg" src="AF7AD254.png" ... 44px"> <img class="sg" src="AC8C2369.png" id="s119_i" title="" alt="TP_tmp.png"

15 Nov 2014: id="s33_i" style="z-index:1;left:0px;top:0px;width:145.84px;height:295.70px" > </div> <div class="sg" id="s29" data-sgid="Rectangle 24" ... data-sgid="Picture 24" style="z-index:7;left:305.35px;top:129.87px;width:390.17px;height:299.92px"> <img class="sg"

10 Dec 2014: 24) for allfive system sizes shown in Table II and also in Fig. ... Data derived from (24) are shown for systems of N particles at n unitsof flux above the ground state Nφ = N 2 n.

15 Mar 2014: Edge Singularity in X-ray Absorption in Metals. 24. Non-equilibrium Superconductivity. 25.

11 Jul 2014: BOOKS. MOVIES. PAINTINGS. 1. A man without qualities. Journey to the end of the night. Les Particules élémentaires. Very little. almost nothing. That palm at the end of the mind. The Passion of Joan of Arc. Japanese girls at the harbour. Der

24 Feb 2014: 0. 5. 10. 15. 20. 25. 18 20 22 24 26 28 30 32 34 36 38.

29 Nov 2014: 24. 6.5 Example: prospecting. 25. 7 Bandit Processes and the Gittins Index 26.

26 Jan 2014: Random Surfaces and Quantum Loewner Evolution. Jason Miller and Scott Sheffield. Massachusetts Institute of Technology. January 23, 2014. Jason Miller and Scott Sheffield (MIT) Random Surfaces and QLE January 23, 2014 1 / 30. Overview. Part I:

1 Oct 2014: Liouville Quantum Gravity as a Mating of Trees. Bertrand Duplantier, Jason Miller, and Scott Sheffield. CEA/Saclay and Massachusetts Institute of Technology. September 30, 2014. Duplantier, Miller, Sheffield Liouville Quantum Gravity as a Mating of

7 Oct 2014: In the limit as 0, we obtain2 the critical space–time percolation process onZ R, see Figure 5.1 and, for example, [24].

13 Jun 2014: Ui′(λi) yi(λ) < 0 (23). U′i(y(λ)) λi > 0 (24). yi(λ)λi. ... Notice the inequality (24), which is satisfied at λi = 0,cannot be sustained for all λi since U′i(y(λ)) is a decreasing function of λi.

14 Aug 2014: However, H o u c k [24] has shown via simulation that it is close to being optimal in m a n y cases.

20 Dec 2014: 3672. 13. I. Steinbach, and M. Plapp: ‘Pearlite revisited’, Continuum Mechanicsand Thermodynamics, 2012, 24, 665–673. ... 24. R. S. Qin, A. Rahnama, W. J. Lu, and B.

20 Dec 2014: relationships [24]. The influence of ausforming condition on the block width ofmartensite for all the conditions is shown in Fig. ... 24. H. Kitahara, R. Ueji, N. Tsuji, and Y. Minamino: ‘Crystallographic fea-tures of lath martensite in low-carbon

14 Feb 2014: 24] J. A. Francis, M. Turski, P. J. Withers: Materials Science and Technology 25 (2009) 325–334. ... Metal-cored Ar2%CO2 18 1.0 24.7 250 23-36. Table 3: Pre-heat and inter-pass temperatures (TI).

6 Dec 2014: 22, 23, 24, 25, 26, 27]. 13. 2 Literature Review. 2.1 Austenite-Pearlite Reaction. ... Therefore,. vB =. (cγαe cγcγα. )(δDBS2. )(24). According to Turnbull’s analysis, the observed growth rate in Seith and.

6 Dec 2014: 10. 2.2.3 Summary. 16. References. 17. 3 Hydrogen Desorption in Single Phase Steel - Ferrite 24. ... ter (a) 6 h, (b) 24 h and (c) 72 h of charging.

6 Dec 2014: 52100 steel as illustrated in Figure 24 (Sakai 2002). 24. Figure 21: Schematic illustration of macroscopic fatigue fracture surface (Sachs. ... tempering temperature. The hardness of martensite for as-quenched, tempered at. 180, 230, and 250 conditions

29 Aug 2014: For directcomparison half of these samples were subjected additionally to tempering at500C for 24 h. ... Materials Scienceand Engineering, 24:85–94, 1976. 9. [35] H. K. D. H.

31 Aug 2014: 0.24. 0.37. 250. 78.6. 2.8671. 0.22. 0.53. Transformation Temp./C. Lattice Parameter / A.

25 May 2014: Sample Measured sa Sample Measured sa 1 0.18 4 0.24 2 0.19 5 0.24 3 0.24 6 0.17. ... 172, pp. 307–313, 1952. [24] G. R. Speich, “The growth of bainite,” Ph.D.

16 Mar 2014: 1.21 1.17 1.27 1.10 1.22. Allotrimorphic 1.26 0.69 0.45 0.24 0.22Ferrite (0.06) (0.03) (0.01) (0.01) (0.01). ... Metal Science,pp. 341–345. [24] Curry, D., 1980. “Comparison Between Two Models ofCleavage Fracture”.

18 Sep 2014: 24] E. Honda, Z. Nishiyama, On the nature of the tetragonal and cubicmartensites, Science Reports of Tohoku Imperial University 21 (1932)299–331. ... 2014)http://dx.doi.org/10.1016/j.scriptamat.2014.07.006. 24.

21 May 2014: 0.83 2.28 0.011 0.008 1.9 0.044 0.12 1.44 0.24 0.11 1.55 0.019 0.023. ... Materials Science and Technology, 29:1166–1173, 2013. [24] F. Katsuki and M.

16 Dec 2014: The issue is now ofincreasing importance given that there are concerted efforts to exploit thesolution strengthening of ferrite using phosphorus as a solute [22–24]. ... Lee: Materials Science &Engineering A A564 (2013) 461–472. [24] S. Hong, J.

24 May 2014: Both can be heat-treated to produce the requirednanostructure, as shown previously [1, 2, 23, 24]. ... Mater. Sci. Tech-nol., 18:279–284, 2002. 28. [24] C. Garcia-Mateo, F. G.

23 Jul 2014: In alloy A with wC = 0.24 wt%, the two-step treatment worsens theductility with the opposite effect observed in alloy B which contains 0.41 wt%carbon. ... Sci. 8 (2004) 259–265. [24] B. C. DeCooman: Curr. Opi. in Sol.

26 Jan 2014: df1 = χ. (. 1 24. i=0. fi. ). dT, with df1 = 0 if MS1 < T. ... df24 = χ. (. 1 24. i=0. fi. ). dT, with df24 = 0 if MS24 < T (4).

25 Nov 2014: Recent research hasshown that even after significant cycling stressing, the austenite films ofnanostructured bainite in the regions of maximum subsurface shear stressdo not stress transform to martensite [24]. ... 24] W. Solano-Alvarez, E. J. Pickering, H

30 Jan 2014: 18. Y. Tomota et al., “Tensile Deformation of Two Ductile Phase Alloys: Flow CFe–Cr–Ni Alloys.” Materials Science and Engineering, 24 (1976), 85 - 94. ... 24. B.C. DeCooman, “Structure–Properties Relationship in TRIP Steels Containing Carbide

25 May 2014: J. Jacques: Current Opinion in Solid State and Materials Science 8 (2004) 259–265.[24] H.

29 Mar 2014: austenitic TWIP steel is reported to be around 6070 % [21-24]. ... 11. [24] M. Koyama, E. Akiyama, and K. Tsuzaki, Scripta Materialia 66 (2012) 947.

24 May 2014: addressed. Alloys of austenitic iron containing large concentrations of manganese (typically 15–20 wt-%) arenow common in research and are commercially available;22–24 they rely on twinning-inducedplasticity (TWIP) to ... Sci. Technol., 2008, 24,

24 May 2014: Mater. Trans. A, 2011, 42A, (9), 2716–2722. [24] V. D. Manvatkar, A. ... Workpiece and tool materials C-Mn 1018 Steel, W-0.4%Re Tool shoulder and pin diameters, mm (15, 18, 21, 24), (7.9, 9.0) Workpiece thickness, mm 6.35,

25 Apr 2014: for C-Mn steels A = 3.8732 µm10s1 and Qgg 400 kJ mol1) [24]. ... occurring during hot deformation and predicting phase structure comparable. 24. to experimental results.

1 Jul 2014: With care, it is possible to reduce residualstresses in critical locations and enhance the fatigue strength of the joint[18–24]. ... 24. C. Miki, and T. Masayuki: ‘Fatigue strength improvement of out-of-plane welded joints of steel girder under

16 Mar 2014: then precisely analyse them.24) Another distinct possibility is the incorporation of otheranalysis techniques, such as optical imaging and hardness measurements, into the same automatedrobotics, thereby yielding further useful information

3 Jul 2014: 0.94 1.78 2.20 1.42 0.24 0.03 1.45 0.1 817 840. ... Metallurgical & Materials Transactions A,31:2431–2438, 2000. [24] V. V. Basabe, J.

29 Aug 2014: at!1313!K!(1040!C)!for!20!min!has!been!reported!to!dissolve!all!the!cementite![24],!a!rod!sample!was!austenitised!at!Tγ=1313!K!(1040!C)!for!30!min,! ... 16! [23]!A!Yonezu,!T!Hara,!T!Kondo,!H!Hirakata,!K!Minoshima:!Materials!Science!and!Engineering!A!2012

13 Aug 2014: 3 1.07549 112.5407 1.64743e-01 38.5 24 [ 5] 12 2 2 2 1.02970 120.6037 5.04710e-02 11.8 8.

30 Aug 2014: 24, pp. 219–228. [11] H. Swahn, P. C. Becker, O. Vingsbo: Metallurgical & Materials Trans-actions A 1976, vol. ... 107–124. [24] K. L. Johnson: Contact Mechanics: Cambridge University Press, Cam-bridge, U.

13 Jul 2014: Others haveconsidered only the NM state in the assessment of carbon [24]. ... Nazarov, T. Hickel, J. Neugebauer: Physical Review B 82 (2010). 224104.[24] A.

26 May 2014: Sample Measured sa Sample Measured sa 1 0.18 4 0.24 2 0.19 5 0.24 3 0.24 6 0.17. ... 172, pp. 307–313, 1952. [24] G. R. Speich, “The growth of bainite,” Ph.D.

22 Oct 2014: entirely unimpaired following stimulation of AnG compared with. vertex, t (44) = 0.24, n.s., d = 0.07, as was cued recall, t. ... higher than their confidence in their correct source recollection of. those items, t (22) = 5.24, p,0.001, d = 1.42, a

31 Mar 2014: Journal of Neuroscience, 24, 4172–4180. Kensinger, E. A., & Schacter, D.