Thermal Analysis of Polymeric Materials
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Appendix 13–Description of Sawtooth-modulation Response |
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Fig. A.13.15
References to Appendix 13
1.Details about the data analysis without Fourier transformation for sawtooth-type temperature-modulated DSC are given in: Hu W, Wunderlich B (2001) Data Analysis Without Fourier Transformation for Sawtooth-type Temperature-modulated DSC. J Thermal Anal Calorim 66: 677–697.
2.A collection of Fourier series for different curves can be seen, for example in: Lide DR, ed (2002/3) Handbook of Chemistry and Physics, 83rd ed. CRC Press, Boca Raton.
3.The TMDSC with Fourier analysis of the melting pentacontane and the calculations using saw-tooth analysis methods are given in the publication: Wunderlich B, Boller A, Okazaki I, Ishikiriyama K, Chen W, Pyda W, Pak J, Moon, I, Androsch R (1999) Temperaturemodulated Differential Scanning Calorimetry of Reversible and Irreversible First-order Transitions. Thermochim Acta 330: 21–38.
Appendix 14–Group Theory, Configuration, Conformation, Numbers 849
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Fig. A.14.3
Fig. A.14.4
Appendix 16 |
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Summary of X-ray Diffraction and Interference Effects
X-ray diffraction and, analogously, the diffraction of other electromagnetic waves, as detailed in Fig. 1.51 is summarized in Fig. A.16.1. A detailed drawing of the constructive and destructive interference is outlined in Fig. 1.54. A variety of typical diffraction patterns are depicted in Figs. 5.69–72, 5.81, 5.82, 6.4, 6.33, 6.63, 6.103, 7.36, and 7.51. Correspondent constructions can be applied to waves of small particles of matter, such as electrons and neutrons. An electron-diffraction pattern is reproduced in Fig. 5.74. Even sound and water waves follow the same principles of diffraction and interference.
Fig. A.16.1
