... 53, 12 6 1 (19 82) 16 . P.F. Green, D.L. Sidebottom, R.K. Brown, J. Non-cryst. Solids 1 72 17 4, 13 53 (19 94) 17 . P.F. Green, D.L. Sidebottom, R.K. Brown, J.H. Hudgens, J. Non-cryst. Solids 23 1, 89 (19 98) 18 . ... L.Neel,J.Phys.Rad. 12 , 339 (19 51) ; J. Phys. Rad. 13 , 24 9 (19 52) ; J. Phys. Rad. 14 , 22 5 (19 54) 25 6 15 Nuclear Methods is given by the Bloch equa...
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... Ferguson, Phys. Rev. Lett 29 , 125 0 (19 72) 46. D. Wolf, Appl. Phys. Letters 30, 617 (1977) 47. D. Wilmer, J. Combet, Chemical Physics 29 2, 143 (20 03) 28 2 15 Nuclear Methods 22 . G. Majer, presented ... = R 1+iωCR , (16.6) where ω =2 ν denotes the angular frequency. Then, the real and imaginary parts of the impedance can be written as Z = R 1+ω 2 R 2 C 2 and Z = ωCR 2 1...
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Diffusion Solids Fundamentals Diffusion Controlled Solid State Episode 2 Part 3 pdf
... Pb [14] [16] [18] [ 12] [19] [20 ] [ 23 ] ∆H [kJ mol −1 ] 21 1 170 165 28 1 26 6 25 7 107 D 0 [10 −4 m 2 s −1 ] 0.78 0.041 0. 027 1 .33 0 .20 5 0.05 0.887 ∆H/k B T m 18.7 16.5 14.8 19.5 17.5 15 .2 21.4 a correlation ... 19 82, p. 558 29 . J. Mullen, Phys. Rev. 124 (1961) 1 7 23 30 . M. Lăubbehusen, H. Mehrer, Acta Metall. Mater. 38 , 28 3 (1990) 31 . Y. Iijima, K. Kimura, K. Hir...
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Diffusion Solids Fundamentals Diffusion Controlled Solid State Episode 2 Part 4 docx
... D 0 /m 2 s 1 5 ì 10 8 (T> ;27 3 K) 4. 4 ì 10 8 2. 9 ì 10 8 0.9 ì 10 8 (T< ;27 3 K) H/eV 0.106 (T> ;27 3 K) 0. 140 0. 043 0.068 (T< ;22 3 K) D D 0 /m 2 s 1 5 .4 ì 10 8 4. 9 ì 10 8 3.7 ì 10 8 H/eV 0. 129 ... (19.6), and (19 . 24 ), b 1 can be expressed as a function of the ratio D ∗ B (0)/D ∗ A (0): b 1 = −18 + 4 D ∗ B (0) D ∗ A (0) f 1 − f 2 4 1 (ω 1 /ω 3 )+ 14 2 f (4...
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Diffusion Solids Fundamentals Diffusion Controlled Solid State Episode 2 Part 5 ppt
... quasicrystals Al 70 Pd 21 Re 9 Al 64 Co 16 Cu 20 Ta 1.6 Te Al 70 Pd 21 Mn 9 Al 71 .5 Co 14 Ni 14 .5 Al 62 Cu 25 TM 13 (TM = Fe, Ru, Os) Al 69.8 Pd 18.1 Mn 12. 3 Ni 17 Ti 41 .5 Zr 41 .5 Al 71 Fe 5 Ni 24 Ga 20 Mg 43 Zn 37 Al 40 Fe 15 Ge 20 Mn 25 Al 37 Cu 10.8 Li 32. 2 Al 43 Mg 43 Pd 14 Zn 64 .2 Mg 26 .4 Ho 9.4 Zn 60.7 Mg 30.6 Y 8.7 Fig. ... 80, 121 9 (20 00) 24...
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Diffusion Solids Fundamentals Diffusion Controlled Solid State Episode 2 Part 6 pot
... scale 3 82 21 Diffusion in Quasicrystalline Alloys 20 . C. Janot, Phys. Rev. B 73, 181 (19 96) 21 . R. Lăuck, Production of Quasicrystalline Alloys and Phase Diagrams,p .22 2 in [4], 20 02 22. C. Beeli, ... Tsai, H. Nakajima, Mat. Sci. A 29 4 29 6, 7 02 (20 00) 37. C. Khoukaz, R. Galler, H. Mehrer, P.C. Canfield, I.R. Fisher, M. Feuerbacher, Mater. Sci. Eng. A 29 4 29 6, 69 7 (20 00...
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Diffusion Solids Fundamentals Diffusion Controlled Solid State Episode 2 Part 7 docx
... D i ∂ 2 C i ∂x 2 + k −1 C s − k +1 C i C V + k 2 C s C I − k +2 C i (25 .3) ∂C s ∂t = D s ∂ 2 C s ∂x 2 D s ≈0 +k +1 C i C V − k −1 C s + k +2 C i − k 2 C s C I (25 .4) ∂C V ∂t = D V ∂ 2 C V ∂x 2 + ... tracer. References 4 07 25 . H. Bracht, MRS Bulletin, June 20 00, 22 26 . P.E. Blăochl,E.Smargiassi,R.Car,D.B.Laks,W.Andreoni,S.T.Pantelides, Phys. Rev. Lett...
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Diffusion Solids Fundamentals Diffusion Controlled Solid State Episode 2 Part 8 pps
... Diusion C eq i D i (Cu)=6.1 ì10 8 exp 1.64 eV k B T m 2 s 1 , (25 .47) C eq i D i (Ag)=4.3 ì10 8 exp 2. 30 eV k B T m 2 s 1 . (25 . 48) C eq i D i (Au)=1.3 ×10 −5 exp − 2. 98 eV k B T m 2 s −1 . (25 .49) These ... 766 20 . U. Găosele, F. Morehead, W. Frank, A. Seeger, Appl. Phys. Lett. 38, 157 (1 981 ) 21 . A. Seeger, W. Frank, Appl. Phys. 27 , 171 (19 82 ) 22 . C....
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Diffusion Solids Fundamentals Diffusion Controlled Solid State Episode 2 Part 9 potx
... Lidiard, Rep. Progr. Phys. 27 , 161 24 0 ( 196 4) 41. W.D. Compton, R.J. Maurer, J. Phys. Chem. Solids 1, 191 ( 195 6) 42. D. Tannhauser, J. Phys. Chem. Solids 5, 22 4 ( 195 8) 27 .1 Fast Silver-Ion Conductors ... Singapore, 199 3 26 . R.J. Friauf, J. Appl. Phys., Suppl. to Vol. 33, 494 ( 19 62) 27 . N. Laurance, Phys. Rev. 120 , 57 ( 196 0) 28 . V.C. Nelson, R.J. Friauf, J. Phys...
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Diffusion Solids Fundamentals Diffusion Controlled Solid State Episode 3 Part 1 doc
... 31 , 17 7 (19 90) 16 . A. Peker, W.L. Johnson, Appl. Phys. Lett. 63, 234 2 (19 93) 17 . X.H. Lin, W.L. Johnson, J. Appl. Phys. 78, 6 514 (19 95) 18 . W.L. Johnson, Mat. Res. Soc. Symp. Proc. 554, 31 1 (19 99) 19 . ... 615 (19 84) 13 . A. Inoue, T. Zhang, T. Masumoto, Mater. Trans., JIM, 33 , 965 (19 90) 14 . A. Inoue, Mater. Trans., JIM, 36 , 866 (19 95) 15 . A. Inoue, T. Zhang,...
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Diffusion Solids Fundamentals Diffusion Controlled Solid State Episode 3 Part 2 pot
... Non-Cryst. Sol. 35 1, 38 16 (20 05) 29 . A.W. Imre, S. Voss, H. Mehrer, Phys. Chem. Chem. Phys. 4, 32 19 (20 02) 30 . S. Voss, F. Berkemeier, A.W. Imre, H. Mehrer, Z. Phys. Chem. 21 8, 135 3 (20 04) 538 30 Diffusion ... atoms. References 5 43 31. Y. Gao, C. Cramer, Solid State Ionics 176, 921 (20 05) 32 . R.J. Charles, J. Amer. Ceram. Soc. 48, 4 32 (1965) 33 . R. Terai, J. N...
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Diffusion Solids Fundamentals Diffusion Controlled Solid State Episode 3 Part 3 pot
... slopes of diagrams like Fig. 32 .14 as sD gb δ =1 .32 2 D t (−∂¯c/∂z 6/5 ) −5 /3 (32 .42) for constant-source conditions and sD gb δ =1 .30 8 D t (−∂¯c/∂z 6/5 ) −5 /3 (32 . 43) for instantaneous-source ... Philib- ert [28]. The first term of Eq. (32 .10) is a complementary error function c 1 = c 0 erfc(η/2) (32 . 13) 32 .3 Diffusion along an Isolated Boundary (Fisher Model) 559 32...
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Diffusion Solids Fundamentals Diffusion Controlled Solid State Episode 3 Part 4 pps
... C: Solid State Physics 14, 38 63 (1981) 11. A.D. Le Claire, A. Rabinovitch, J. Phys. C: Solid State Physics 15, 33 45 (1982), erratum 5727 12. A.D. Le Claire, A. Rabinovitch, J. Phys. C: Solid State ... Defect and Diffusion Forum 95–98, 39 3 40 4 (19 93) 35 . J. Sommer, Chr. Herzig, J. Appl. Phys. 72, 2758–2766 (1992) 36 . A.D. Le Claire, Brit. J. Appl. Phys. 14, 35 1 (19 6...
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Diffusion Solids Fundamentals Diffusion Controlled Solid State Episode 3 Part 5 pps
... Electochem. Soc. 134 , 152 4 (1987); Progr. in Solid State Chemistry 23, 171 (19 95) ; Solid State Ionics 131 , 13 (2000) 66. W. Puin, P. Heitjans, Nanostruct. Mater. 6, 8 85 8 (19 95) 67. W. Puin, S. ... Ni 3 Al as a function of composition at 0. 75 T m from [39 ] 35 6 20. 15 Self-diffusion in L1 2 structured Ni 3 Alaccordingto [39 ] 35 7 20.16 Self-diffusion in the L1 2 inte...
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Diffusion Solids Fundamentals Diffusion Controlled Solid State Episode 3 Part 6 docx
... 504, 5 06, 510, 5 23, 598 Cu 3 Au rule 36 5, 36 6 majority element 36 6 minority element 36 6 cylindrical coordinates 32 D0 3 inremetallics 36 7 D0 3 intermetallics 35 7 Cu 3 Sn 35 8 D0 3 Fe 3 Si 35 8 sublattice ... 457 anelasticity 237 , 239 anisotropic media 33 anisotropy ratio 30 8 Arrhenius diagram 127, 2 46, 287, 289, 30 1, 30 4, 31 7, 33 2, 33 3, 3...
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