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Additional info for Advances in Joining of Ceramics, Volume 138
Lee, E. D. Case, and J. , "The Steady-State Temperature as a Function of Casket Geometry for Microwave-Heated Refractory Caskets," Materials Research Innovations, 1 : 101-116,1997. 38. Traub, K. Y. Lee, and E. D. Case, " The Effect of Casket Geometry on Microwave Heating and Its Modeling", pp. , Westerville, OH, 1998. 39. Y. Lee and E. D. Case, "Steady-State Temperature of Microwave-Heated Refractories as a Function of Microwave Power and Refractory Geometry," Materials Science and Engineering, A269: 8 - 20,1999.
Y. Lee, E. D. Case, and J. , "Microwave Sintering of Ceramic Matrix Composites and the Effect of Organic Binders on the Sinterability," Proceedings of 11th Annual Advanced Composites Conference, The Engineering Society, Ann Arbor, MI, 491-504,1995. 28. Y. Lee, P. H. Dearhouse, and E. D. Case, "Microwave Sintering of Alumina Using Four Different Single-Cavity Modes," Journal of Materials Synthesis and Processing, 7: 159 -166,1999. 29. K. Y. Lee and E. D. Case, "Microwave Sintering of Alumina Matrix Zirconia Composites Using a Single-Mode Microwave Cavity," Journal Materials Science Letters, 18: 201-203,1999.
55 Advances in Joining of Ceramics 38 It is insightful to assume that the toughness of the layer that contains the crack is fixed, and to examine how the crack kink angle depends the various parameters when toughness is constant. Figure 4 shows the crack kink angle as a function of layer thickness for three values of toughness for the 5-layer configuration. 5 mm, the kink angle appears not to depend strongly on toughness and is close to zero. 5 mm. It is also clear that the dependence of crack kink angle on layer thickness is much stronger for the less tough layer.
Advances in Joining of Ceramics, Volume 138