kinetics of materials r balluff s allen w carter wiley 2005 potx

... mathematics and physics. Extensive discussion of mechanisms is therefore a feature of this book. We stress rigorous analysis, where possible, and try to build a foundation for un- derstanding kinetics ... the requisite tools for understanding most of the major aspects of kinetic processes in materials. 1.1 THERMODYNAMICS AND KINETICS In the study of materials science,...

Ngày tải lên: 27/06/2014, 23:20

... references and index. ISBN 13 97 8-0 -4 7 1- 2 468 9-3 ISBN -1 0 0-4 7 1- 2 468 9 -1 1 .Materials- Mechanical Properties. 2. Materials science I. Allen, Samuel M. 11 . Carter, W. Craig. 11 1. Kemper, Rachel A. ... old-newJ’old - - J’old - - Anew-oldXnewAold-new*ld 4 4- Therefore, Aold-new old new-rold xnew = - XA x- - XA and (1. 32)...

Ngày tải lên: 11/08/2014, 10:22

... eigenvalues are -1 .27 2 52 -0 .871 722 0.14 423 8 01 = [ -0 .5:8613 ] 21 2 = [ -2 .413084 ] w3 = [ -0 .03105511 ] (1.57) Note that these eigenvectors are of arbitrary length. 42 CHAPTER ... - eq (2. 51) - - Bibliography 1. F.C. Larch6 and J .W. Cahn. A linear theory of thermochemical equilibrium of solids under stress. Acta...

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... D22 0 23 0 13 0 23 033 -g[ :::I -9 [ :::I -9 [ I,I] (4.84) Because of the cubic crystal symmetry, the fluxes parallel to the directions of the gra- dients in the three cases (i.e., -gD11, ... ffxx + ffyy + ffzz - ff1.7. + 066 + ffzz p =- (3. 80) 3 3 p(1+ v)b sine - p(1 + v)b y - - - 3~ (1 - U) T 3~ (l - V) x2 +...

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... D2 1 Jp = - J1 - A 52 Dll- D22 - A 2A and -0 21 Dll- D22 +A c2 c1 + 2A c, = - A Dll - D22 - A 2A c2 D2 1 cp =-c1 - A (6.32) (6.33) (6. 34) (6.35) The ... local thermal equilibrium at very small concen- trations. Kinetics of Materials. By Robert W. Balluffi, Samuel M. Allen, and W. Craig Carter. 131 Copyright...

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... 3. W. Schilling. Self-interstitial atoms in metals. J. Nucl. Mats., 6 9-7 0( 1-2 ): 46 5-4 89, 1978. 4. P. Shewmon. Diffusion in Solids. The Minerals, Metals and Materials Society, War- ... characteristic of the crystalline state no longer exists. Good bulk material is free of line or planar imperfections. Kinetics of Materials. By Robert W. Ball...

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... 68(15):234 7- 2 349, 1992. 17. K. Ratzke, A. Heesemann, and F. Faupel. diffusion in Fe39Ni40B21 glass. J. Phys. Condens. Matter, 7( 39) :76 6 3 -7 668, 1995. The vanishing isotope effect of cobalt 18. R .S. ... size in amor- phous Ni-Zr. Phys. Rev. B, 37( 11):653 3-6 535, 1988. 26. R. Kirchheim. Interstitial diffusion in glass. Defect and Diffusion Forum, 9 5-9 8:...

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... bicrystals. Sow. Phys. Solid State, 23(10):171 8-1 721, 198 1. 22. R .W. Siegel, S.M. Chang, and R .W. Balluffi. Vacancy loss at grain-boundaries in quenched polycrystalline gold. Acta Metall. Muter., ... and R .W. Balluffi. Direct observation of grain boundary dis- location climb in ion-irradiated gold bicrystals. Phil. Mag., 26:23 9- 2 52, 197 2. 25. K.E. Rajab and R.D. Do...

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... [l] and Wagner [2]. Most of the Kinetics of Materials. By Robert W. Balluffi, Samuel M. Allen, and W. Craig Carter. 363 Classical Mean-Field Theory of Coarsening * Copyright ... Lett., 58(6):27 1-2 75, 1988. 27. J.A. Glazier, S.P. Gross, and J. Stavans. Dynamics of two-dimensional soap froths. Phys. Rev. A, 36(1):30 6-3 12, 1987. 28. W .W. Mullins. O...

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... R.B. Heady and J .W. Cahn. An analysis of capillary force in liquid-phase sintering of spherical particles. Metall. Trans., 1(1):18 5-1 89, 1970. J .W. Cahn and R.B. Heady. Analysis of ... need to be considered. Kinetics of Materials. By Robert W. Balluffi, Samuel M. Allen, and W. Craig Carter. 419 Copyright @ 2005 John Wiley & Sons, Inc. PART...

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... morphologically unstable). Other types of growth are treated elsewhere in this book. Kinetics of Materials. By Robert W. Balluffi, Samuel M. Allen, and W. Craig Carter. 501 Copyright 0 2005 ... answer. -yc = 160 mJ m-2 7' = 800 mJ m-2 AgE = 2.6 x lo9 J m-3 AgB = 8 x lo6 (T - 900K) J m -3 K-' (coherent interface) (incoherent inte...

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... faceting of surface, 347, 60 9-6 10 Fe, 30, 167, 169, 192, 206, 221, 317, 579 Fe-A1, 451, 456 Fe-C, 69, 566 Fe-C-Si, 69 FeCr. 451 Fe-Crko, 451 Fe-Mo, 451, 456 Fe-Ni. 57 4-5 75. 57 8-5 80 FeNi-C, ... algebraic signs of, 53, 435 anisotropy of, 88 definition of, 42 interdiffusivity, 4 9-5 0, 5 3-5 4, 87 in spinodal region, 43 3-4 35 intrinsic, 47, 5 3-5 4 s...

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... Grain-Boundary Diffusion 9.2 .1 9.2.2 9.2.3 14 1 14 1 14 1 14 5 14 5 14 6 14 8 14 9 15 4 15 5 15 6 15 8 15 8 15 9 16 3 16 3 16 4 16 4 16 5 16 7 16 7 16 9 16 9 17 7 18 3 18 3 18 9 18 9 19 0 209 ... (1. 58) 1 1 1 -1 .27252 -0 .8 717 22 0 .14 4238 1 1 1 - P= [ -0 .538 613 -2 .43084 -0 .0305 511 The inverse of may be calculate...

Ngày tải lên: 13/08/2014, 05:20

... LW 4- (2. 28) will arise. The existence of the force Fq indicates the presence of a gradient in the electrical potential, V4, along the bar. Therefore, using Eqs. 2. 28 and 2. 26, LQQ ... then Eq. 2. 15 reduces to TU =-& amp;.Vc$ (2. 52) Using Ohm's law, & = -pV4, TU = p 10c$l2 (2. 53) Because U 2 0 and lVc$ 12 is positive, p must...

Ngày tải lên: 13/08/2014, 05:20

... ff 13 p11 pl2 p 13 ff2l ff22 ff 23 p2l p22 p 23 a31 a32 ff 33 p31 p32 p 33 711 712 7 13 711 v12 7 13 721 722 7 23 721 722 77 23 . 731 732 733 731 v32 v 33 (4.79) (b) Onsager's ... D22 0 23 0 13 0 23 033 -g[ :::I -9 [ :::I -9 [ I,I] (4.84) Because of the cubic crystal symmetry, the fluxes parallel to the directions of the gr...

Ngày tải lên: 13/08/2014, 05:20