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  1. Results that match 2 of 3 words

  2. CHAPTER 6 FURTHER PREDICTIONS ABOUT WELD METAL STRENGTH 6.1 ...

    www.phase-trans.msm.cam.ac.uk/2007/Sugden/Ch6.pdf
    7 Jun 2010: Thewlis, 1987 22A11 191 558 307 0.25 0.04 0.71tI 22A12 195 569 308 0.23 0.02 0.75tI 22A13 191 558 308 0.24 0.01 ... 802 202 590 343 0.24 0.62 0.1411 803 188 549 335 0.11 0.74 0.1511 804 184 537 329 0.18 0.63 0.19.
  3. Slide 1

    www.phase-trans.msm.cam.ac.uk/2005/TrendsPresentation.ppt
    7 Jun 2010: 91.55. 2.8. 54.1. 72.7. 91.8. 400. 101.24. 3.2. 54.1. 72.7. 91.8. ... 54.1. 72.7. 91.8. 350. 91.55. 2.8. 54.1. 72.7. 91.8. 400. 101.24.
  4. paper_revised.dvi

    www.phase-trans.msm.cam.ac.uk/2009/MoB.pdf
    7 Jun 2010: Progress inMaterials Science, 29:321–386, 1985. [24] J. W. Christian. Theory of Transformations in Metal and Alloys, Part I. ... Khan. Incomplete reaction phenomenon inhigh-strength bainitic steels. Metallurgical and Materials Transactions A,
  5. 1 NEW CREEP RUPTURE ASSESSMENT OF GRADE 91 L. ...

    www.phase-trans.msm.cam.ac.uk/2005/LINK/162.pdf
    7 Jun 2010: 1 2 1 59 2 61 2.9630 16 5 2 2 20 5 25 1.0637 1 1 1 0.0640 24 5 2 31 31 1.5645 3 3 ... TOTAL 1657 37 220 29 92 28 52 8 24 20 5 16 3 4 2053 142 2195 100.
  6. is430777

    www.phase-trans.msm.cam.ac.uk/2003/mobility.pdf
    7 Jun 2010: Fig. 3. Particles alignment along the extrusion direction. ic because of the strong alignment of the yttria particlesalong the extrusion direction.24–26) The particles hinderboundary motion more effectively in the ... H. Bhadeshia:Metall. Trans. A, 24
  7. MICROSTRUCTURAL STABILITY OF STRONG 9–12 wt% Cr STEELS H. ...

    www.phase-trans.msm.cam.ac.uk/2005/Rome2.pdf
    7 Jun 2010: These include localrecrystallisation due to the presence of coarse carbides at the prior austenite grain boundaries [24]and impurity effects. ... 24] K. KIMURA, H. KUSHIMA, F. ABE and K. YAGI, Materials Science and Engineering,A234–236 (1997)
  8. (ICOMAT02 Christian)

    www.phase-trans.msm.cam.ac.uk/2002/Christian.pdf
    7 Jun 2010: Such a transformation hasbeen called diffusional–displacive transformation [23,24]. This does not negate the consequences. ... S. A. (1984) 293–326.[24] Christian, J. W. Progress in Materials Science 42 (1997) 109–124.[25] Christian, J.
  9. 26 Jul 2010: K. D. H. Bhadeshia: Mater. Sci. Technol.,. 2008, 24, 343–347. 18. ... Ann., 1952, 136, 25–37. 24. M. Hillert: ‘Paraequilibrium’, Technical report, Swedish Institute.
  10. D:/Sangeeta/Sc_Exptal/Paper2-Compromise on properties/Paper2 Revised…

    www.phase-trans.msm.cam.ac.uk/2010/khare/khare.pdf
    7 Jun 2010: 0γ = 0.24 retained. was calculated using the Koistinen and Marburger equation [44]. ... 42, pp. 20–24. [4] Y. Tomita: Materials Science and Technology 1991, vol.
  11. INNOVATION OF CONVENTIONAL HEAT TREATMENT AND MICROSTRUCTURAL…

    www.phase-trans.msm.cam.ac.uk/2005/LINK/126.pdf
    7 Jun 2010: Since 1990s, high magnetic field has been introduced into various solid-state phase transformations, such as transformation from austenite to ferrite and its reverse [22-24], and other diffusional transformations. ... 51, (2003), p.2921. [24] H. OHTSUKA,

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