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Table 3-2 cont’d:  Calculation of critical nucleation parameters and nucleation rate at zero internal and externally applied
                             stress. Case of finite energy barrier model of solvus hysteresis - equilibrium solvus assumed to be given
                             midway between TSSD and TSSP2 solvi [Pan et al., 1996].

                   gstrain(  gstrain(re  ao*(m)  co*(m)  Vo*(nu  i(J/  =c/  Go*   exp(-  *(s -  no*( nu  Jo(nucl
                                                      3
                                                                                                      3 -1
                                                                                                3
                                                            2
                   exact)   duced)         =∙a*   cl,m )   m )   i          Go*/kBT  1 )   cl/m )   /m s )
                                                                              n)
                   1.94E+  1.94E+07  4.317  8.203E  6.405E  0.2   0.01  4.451  8.11728E  1.14E  3.54E-  4.04E+
                   07                E-09   -11    -27           90    E-19   -26      +04   03      00
                   2.59E+  2.59E+07  3.396  8.604E  4.157E  0.15   0.02  2.754  2.98249E  7.07E  1.30E  9.19E+
                   07                E-09   -11    -27           53    E-19   -16      +03   +07     09
                   3.88E+  3.88E+07  2.509  9.533E  2.513E  0.1   0.03  1.503  3.38214E  3.86E  1.47E  5.69E+
                   07                E-09   -11    -27           80    E-19   -09      +03   +14     16
                   4.85E+  4.85E+07  2.183  1.037E  2.070E  0.08   0.04  1.138  3.84287E  2.92E  1.68E  4.89E+
                   07                E-09   -10    -27           75    E-19   -07      +03   +16     18

                   5.54E+  5.54E+07  2.038  1.106E  1.924E  0.07   0.05  9.914  2.57559E  2.55E  1.12E  2.86E+
                   07                E-09   -10    -27           43    E-20   -06      +03   +17     19
                   5.96E+  5.96E+07  1.973  1.153E  1.881E  0.06  0.05  9.294  5.75676E  2.39E  2.51E  5.99E+
                   07                E-09   -10    -27     5     85    E-20   -06      +03   +17     19
                   6.45E+  6.45E+07  1.917  1.214E  1.868E  0.06   0.06  8.771  1.13632E  2.25E  4.95E  1.12E+
                   07                E-09   -10    -27           33    E-20   -05      +03   +17     20
                   7.03E+  7.03E+07  1.872  1.294E  1.900E  0.05  0.06  8.372  1.90763E  2.15E  8.32E  1.79E+
                   07                E-09   -10    -27     5     91    E-20   -05      +03   +17     20

                   7.72E+  7.72E+07  1.848  1.404E  2.008E  0.05   0.07  8.152  2.53804E  2.09E  1.11E  2.32E+
                   07                E-09   -10    -27           60    E-20   -05      +03   +18     20
                   8.57E+  8.57E+07  1.856  1.567E  2.262E  0.04  0.08  8.225  2.30658E  2.11E  1.01E  2.12E+
                   07                E-09   -10    -27     5     44    E-20   -05      +03   +18     20
                   1.27E+  1.27E+08  2.891  3.663E  1.283E  0.03   0.12  1.996  5.57495E  5.13E  2.43E  1.25E+
                   08                E-09   -10    -26           67    E-19   -12      +03   +11     14
                   1.36E+  1.36E+08  3.757  5.098E  3.014E  0.02  0.13  3.370  1.0074E-  8.65E  4.39E  3.80E+
                   08                E-09   -10    -26     8     57    E-19   19       +03   +03     06
                   1.41E+  1.41E+08  4.625  6.509E  5.831E  0.02  0.14  5.107  1.62364E  1.31E  7.08E-  9.28E-
                   08                E-09   -10    -26     7     07    E-19   -29      +04   07      04
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