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Table 3-3 cont’d:  Calculation of critical nucleation parameters and nucleation rate at zero internal and externally applied
                             stress. Case of accommodation energy model of solvus hysteresis - equilibrium solvus assumed to be
                             given by TSSD solvus [Pan et al., 1996].

                   gstrain(  gstrain(re  ao*(m)  co*(m)  Vo*(nu  i(J/  =c/  Go*   exp(-  *(s )  no*(nu  Jo(nucl/
                                                                                          -1
                                                                                                      3 -1
                                                            2
                                                                                                 3
                   exact)   duced)         =∙a*   cl,m )   m )   i         Go*/kBT         cl/m )   m s )
                                                      3
                                                                             n)
                   3.17E+  3.17E+07  2.994  9.280E  3.483E  0.2   0.03  3.491  2.0821E-  5.49E  9.08E  4.98E+
                   07                E-09   -11    -27           10    E-19   20       +03    +02    05
                   4.22E+  4.22E+07  2.370  9.794E  2.304E  0.15   0.04  2.187  4.6596E-  3.44E  2.03E  6.99E+
                   07                E-09   -11    -27           13    E-19   13       +03    +10    12
                   6.32E+  6.32E+07  1.775  1.101E  1.453E  0.1   0.06  1.228  1.1938E-  1.93E  5.20E  1.01E+
                   07                E-09   -10    -27           20    E-19   07       +03    +15    18
                   7.87E+  7.87E+07  1.565  1.213E  1.244E  0.08   0.07  9.537  4.1996E-  1.50E  1.83E  2.75E+
                   07                E-09   -10    -27           75    E-20   06       +03    +17    19

                   8.98E+  8.98E+07  1.475  1.307E  1.192E  0.07   0.08  8.480  1.6555E-  1.33E  7.22E  9.63E+
                   07                E-09   -10    -27           86    E-20   05       +03    +17    19
                   9.66E+  9.66E+07  1.438  1.372E  1.189E  0.06  0.09  8.061  2.854E-  1.27E  1.24E  1.58E+
                   07                E-09   -10    -27     5     54    E-20   05       +03    +18    20
                   1.04E+  1.04E+08  1.410  1.457E  1.212E  0.06   0.10  7.741  4.3253E-  1.22E  1.89E  2.30E+
                   08                E-09   -10    -27           33    E-20   05       +03    +18    20
                   1.1367  1.14E+08  1.393  1.570E  1.276E  0.05  0.11  7.559  5.4734E-  1.19E  2.39E  2.84E+
                   E+08              E-09   -10    -27     5     27    E-20   05       +03    +18    20

                   1.25E+  1.25E+08  1.396  1.731E  1.414E  0.05   0.12  7.595  5.2271E-  1.19E  2.28E  2.72E+
                   08                E-09   -10    -27           40    E-20   05       +03    +18    20
                   1.38E+  1.38E+08  1.435  1.977E  1.705E  0.04  0.13  8.022  3.0023E-  1.26E  1.31E  1.65E+
                   08                E-09   -10    -27     5     78    E-20   05       +03    +18    20
                   1.55E+  1.55E+08  1.547  2.398E  2.403E  0.04   0.15  9.321  5.5568E-  1.47E  2.42E  3.55E+
                   08                E-09   -10    -27           50    E-20   06       +03    +17    19
                   1.75E+  1.75E+08  1.852  3.281E  4.716E  0.03  0.17  1.337  2.9145E-  2.10E  1.27E  2.67E+
                   08                E-09   -10    -27     5     71    E-19   08       +03    +15    17
                   2.03E+  2.03E+08  3.058  6.320E  2.476E  0.03   0.20  3.643  2.8785E-  5.73E  1.25E  7.19E+
                   08                E-09   -10    -26           67    E-19   21       +03    +02    04
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