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By Joseph Lipka

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The system. The viscosity values begin to drop dramatically at approximately 990°C and at approximately 1190°C the rate of decreasing viscosity lowers. The minimum in viscosity is reached at approximately 1200°C. The region in which viscosity is low is in the same time frame as when a significant amount of deformation occurs. Figure 15 also shows the dependence of stress on densification of the samples. Viscosity was calculated and plotted using both instantaneous stress (instantaneous density and dimensions) and constant stress (using fired density and dimensions).

The pyroplastic index is defined as the deformation at a stress of 50 W a and successfully demonstrates the tendency of a body to deform. :s+ ++ ++ 1400 1200 1000 V i i t y calculated using instantaneous values of stress CI V i m i t y calculated L s i n g constantstress 50 100 150 2 $ E 400+ 88 0 5 Y 800 W 8eeee -Y 200 200 0 250 Time (minutes) Figure I 5. Calculated system viscosity using the steady-state creep equation. mation events take place. The mechanisms are both due to viscous flow, but occur at much different rates.

Seidermann, and A. Baumgarten, “The Formation of Casting Pores in Slip Cast Products: Means of Prevention,” CFI/Berichte DKG, 67 [6] 239 (1990). 3 . D. ” Ceram research paper 749, 1987. 4. W. M. Sigmund, “Novel Powder-Processing Methods for Advanced Ceramics,” J. Am. Ceram. ,83 [7] 1557-1574 (2000). 5. F. H. Baader, T. J. Graule and L. J. Gauckler, “Direct Coagulation Casting - A New Green Shape Technique, Part 11: Application to Alumina,” Indust. , 16 [ 11 (1996). 6. R. M. Sambrook, J. G. P. Binner, J.

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