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Book/Report | FZJ-2018-02655 |
; ;
1986
Kernforschungsanlage Jülich, Verlag
Jülich
Please use a persistent id in citations: http://hdl.handle.net/2128/18286
Report No.: Juel-2056
Abstract: Arguements are presented showing that the resistance to thermal stressing ("thermal shock") under pulsed thermal energy deposition by various kinds of beam irradiations is approximately proportional to $\phi \sqrt{tp}$, where $\phi_{a}$ is the absorbed power density and tp is the pulse length, under conditions of diffusivity controlled spreading of heat. In practical beam irradiation testing, incident power density, $\phi$, is reported. To evaluated the usefulness of $\phi \sqrt{tp}$ as an approximation to $\phi \sqrt{tp}$, damage threshold values are reviewed for different kinds of beams (electron, proton, and laser) for a range of tp values 5x10$^{-6}$ to 2s. Ruby laser beam irradiation tests were made on the following ceramics : AIN, BN, graphite, $\alpha$-SiC, $beta$-SiC coated graphites, ($\alpha + \beta$)Si$_{3}$N$_{4}$, CVD (chemical vapor deposition) TiC coated graphite, CVD TiC coated Mo, and CVD TiN coated IN 625. The laser beam pulse lengths investigated were 9x10$^{-4}$ (normal) and 5x10$^{-6}$s (saturable dye Q-switched) and the power densities ranged from 25 to 4000 kW/cm$^{2}$ corresponding to $\phi \sqrt{tp}$ values of 0.8 to 8.8 kJ/cm$^{2}$s$^{1/2}$.
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