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Interplay of Modelling Techniques www.msm.cam.ac.uk/phase-trans.

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Presentation on theme: "Interplay of Modelling Techniques www.msm.cam.ac.uk/phase-trans."— Presentation transcript:

1 Interplay of Modelling Techniques

2

3 materials modelling Pettifor

4 0.4 C 2 Si 3 Mn wt% 1 µm

5 50 µm

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7

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9 U.K.

10 Fe-2Si-3Mn-C wt% 800 B 600 Temperature / K 400 M 200 0.2 0.4 0.6 0.8 1
0.2 0.4 0.6 0.8 1 1.2 1.4 Carbon / wt%

11 Fe-2Si-3Mn-C wt% 1.E+08 1 month Time / s 1.E+04 1.E+00 0.5 1 1.5
1 year 1 month Time / s 1.E+04 1.E+00 0.5 1 1.5 Carbon / wt%

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13 g g a a a 200 Å

14 Stress / GPa Velocity km s-1 Hammond and Cross, 2004

15 GRP mild steel “superbainite” vehicle steel Peter Brown (DSTL)
Dave Crowther (QinetiQ)

16 “more serious battlefield threats”

17 ballistic mass efficiency
consider unit area of armour

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19 Phase diagrams

20 Generalised models (binary)
Hillert, Kaufman, Kubachewski

21 Ternary approximation

22 Ternary interactions

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25 Lengthening rate / m s-1 Te Temperature / °C Bhadeshia, 1985

26 Solution models Quasichemical approximation, atoms are not distributed at random. Pairs of atoms are treated as independent entities

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30 Reference state Chen, Hansip & Bhadeshia, 2004

31 Distant and near-neighbours

32 -0.17 eV 2.17 eV Chen, Hansip & Bhadeshia, 2004

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35 Kirkaldy, 1968

36 Siller and McLellan, 1969

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38 Bhadeshia, 1981

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41 anitferromagnetic ground state
Weiss and Tauer

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43 Kaufman

44 French National Railways
(Howard Smith)

45 tallest building in the world earthquakes

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47 cooling of constrained tensile specimen

48 Variables C, Mn, Si, Ni, Cr, Mo, V, Co, B, N, O…..
Thermomechanical processing of steel Welding consumable Welding parameters Subsequent heat treatment

49 ESRF Synchrotron

50 Synchrotron studies

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53 critical stress intensity
Charpy fatigue tensile critical stress intensity corrosion

54 non-linear functions

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56 Keehan et al., 2004

57 Fusion Power light nuclei combine into heavier nuclei
Same process as occurs in the sun Produces heat Releases neutrons Combination of deuterium and tritium into helium (alpha particles) and neutrons - at 14 MeV Neutrons escape plasma (uncharged) and so are absorbed by the reactor walls - releasing heat.

58 steel to resist damage from fast neutrons
low-activation

59 Kemp, Cottrell and Bhadeshia, 2005

60 Kemp, Cottrell, Bhadeshia, Odette, Yamamoto and Kishimoto, 2005

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