Microstructural Evolution of Aluminum During the Course of High Temperature Creep
Microstructural Evolution of Aluminum During the Course of High Temperature Creep
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The pattern of Laue spots is apparently the result of the super- position of the diffraction spots from only a few crystal- line elements or subgrains. Quantitative metallographic measurements of the corresponding creep specimen, S5-43, have shown that at the end of precreep the sub grain boundary area is small, Figure 89(a), and the fraction of grains con- taining subgrains is also small, Figure 90(a). Two hours after the beginning of the temperature increase, the Laue photograph of Figure 100... shows that the pattern observed at the end of precreep has begun to disappear and that short segments of Debye rings have formed. The faint spots corre^ sponding to a single crystal exhibit asterism; therefore some lattice bending does exist. This corresponds to an increase in the subgrain boundary area and an increase in the fraction of grains containing subgrains shown previously in Figures 89(a) and 90(a), respectively. With continued creep at the higher temperature, the Laue photograph of Figure 101(a) shows an increase in the length of Debye ring segments and the complete disappearance of the superimposed single crystal patterns observed in Figure 99.
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To quickly assess the difficulty of the text, read a short excerpt:
The pattern of Laue spots is apparently the result of the super- position of the diffraction spots from only a few crystal- line elements or subgrains. Quantitative metallographic measurements of the corresponding creep specimen, S5-43, have shown that at the end of precreep the sub grain boundary area is small, Figure 89(a), and the fraction of grains con- taining subgrains is also small, Figure 90(a). Two hours after the beginning of the temperature increase, the Laue photograph of Figure 100... shows that the pattern observed at the end of precreep has begun to disappear and that short segments of Debye rings have formed. The faint spots corre^ sponding to a single crystal exhibit asterism; therefore some lattice bending does exist. This corresponds to an increase in the subgrain boundary area and an increase in the fraction of grains containing subgrains shown previously in Figures 89(a) and 90(a), respectively. With continued creep at the higher temperature, the Laue photograph of Figure 101(a) shows an increase in the length of Debye ring segments and the complete disappearance of the superimposed single crystal patterns observed in Figure 99.
What to read after Microstructural Evolution of Aluminum During the Course of High Temperature Creep?
You can find similar books in the "Read Also" column, or choose other free books by Connell, Richard Grant, 1938- to read onlineMoreLess
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