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J Therm Anal Calorim 56:755–761 ˇ ak J (2000) Kinetic modeling of advanced inorganic glass-ceramics formation 103. Koga N, Sest´ by crystal growth from pre-existing nuclei. J Therm Anal Calorim 60:667–674 ˇ ak J (2000) Crystal nucleation and growth in lithium diborate glass by thermal 104. Koga N, Sest´ analysis. J Am Ceram Soc 83(7):1753–1760 ˇ ak J (2000) Thermogravimeric analysis 105. Mamleev V, Bourbigot S, LeBras M, Duquesne S, Sest´ of multistage decomposition of materials. Phys Chem Chem Phys 2:4796–4803 106.
Broido A, Williams AF (1970) Use of asymptotic analysis of the large activation energy limit to compare various graphical methods of treating TG data. Thermochim Acta 6:245–253 92. Koga N (1997) Physico-geometric kinetics of solid-state reactions by thermal analysis. J Therm Anal 49:45–56 ˇ ak–Berggren equation a general expression of kinetic 93. M´alek J, Criado JM (1991) Is the Sest´ models? Thermochim Acta 175:305–309 ˇ ak J, Militk´y J (1989) Boundary conditions of kinetic models. 94. M´alek J, Criado JM, Sest´ Thermochim Acta 153:429–432 ˇ ak J (1992) Evaluation and interpretation of nonisothermal kinetic models.
10), where the value integrated from 0 to t at the selected ˛ of the respective data points on the plane will be the constant value of g(˛)/A. Using this relationship, the value of Ea can be determined by a numerical optimization method of minimizing the deviation of the Ea values evaluated for the respective data points [76, 77]. In the integral method, the linear regression analysis for the isoconversional relationship can be applied only for the series of kinetic data recorded under isothermal or linearly increasing temperatures.