Download e-book for iPad: ADVANCES IN CERAMICS ARMOR VI: Ceramic Engineering and by Swab, Sanjay Mathur, Tatsuki Ohji
By Swab, Sanjay Mathur, Tatsuki Ohji
The Armor Ceramics Symposium used to be held January 25-27, 2010 in
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Extra resources for ADVANCES IN CERAMICS ARMOR VI: Ceramic Engineering and Science Proceedings, Volume 31
The Beer-Lambert law is then used to calculate the attenuation coefficient at each frequency, using the first bottom surface reflection as the initial intensity and the second bottom surface reflection as the intensity after propagation. This law is stated as: (1) If testing is performed in pulse-echo configuration, the path length is defined as twice the thickness of the sample. Figure 1 illustrates an oscilloscope view of labeled peak reflections showing the width of the time window used when performing the FFT on reflected signals.
Cook, and A. DiGiovanni, Transparent Spinel Fabricated from Novel Powders: Synthesis, Microstructure, and Optical Properties, 10th DoD Electromagnetic Windows Symposium,(2004). 3 K. Rozenburg, I. Riemanis, H. Kleebe, and R. Cook, Sintering Kinetics of a MgAl204 Spinel Doped with LiF, J. Am. Soc, 91 , 4 4 4 ^ 5 0 (2008). 4 H. Palmour, Development of Polycrystalline Spinel for Transparent Armor Applications, Final Technical Report, Army Materials and Mechanics Research Center, Massachusetts (1972).
Note that a slightly wider scale is used in Figure 4 relative to Figure 2. This accounts for the higher attenuation coefficient values seen in Region 1 due to the large and visible precipitate located there. 6μηι mean grain size. The scale used is in units of dB/cm. όμηι grain size spinel are shown in Figure 5. 5um grain size spinel, attenuation spectra from this material are approximately Gaussian in shape. The results of curve fitting a single Gaussian to each attenuation coefficient spectra can be seen visually in Figure 5 as the dashed lines.
ADVANCES IN CERAMICS ARMOR VI: Ceramic Engineering and Science Proceedings, Volume 31 by Swab, Sanjay Mathur, Tatsuki Ohji