By Hassanein, A.; Morozov, V.; Argonne National Lab.; United States. Dept. of Energy.; United States. Dept. of Energy. Office of Scientific and Technical Information

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Detailed models of macroscopic erosion under IFE cavity conditions are currently being developed and implemented in the HEIGHTS-IFE package. 14. Conclusions Models have been developed to study the dynamic behavior of ICF cavities following target implosions. These models take into account energy deposition from the reflected laser light, emitted photons, neutrons, and target ion debris and the interaction/thermal evolution of chamber gas/wall components. The models are implemented in the comprehensive HEIGHTS-IFE package.

11 MJ Hdebris yield). Additionally, the total vaporization flux is also shown. As seen from the figure for graphite, physical erosion is at least two orders of magnitude lower than chemical erosion and RES. Figure 23 compares the chemical, radiation-enhanced sublimation, and physical sputtering to incident particle flux of carbon and tungsten. Graphite Tungsten Figure 22. HEIGHTS-IFE calculation of physical, chemical, and RES erosion and vaporization Graphite Tungsten Figure 23. HEIGHTS-IFE calculation of total wall erosion 13.

All these thermophysical properties are functions of the local temperature. The boundary conditions are that Ts(x,t) → Tb = constant at large depth distances x, and that on the surface x=0, 27 F (t ) = −k s (Tv ) ∂Ts + ρ s (Tv ) Lv v(Tv ) + σ Tv4 − T04 , where ∂x ( ) Tv (t ) = Ts (0, t); Lv − latent heat; v(Tv ) − velocity of the receding surface. The velocity of the receding surface is a function of the instantaneous surface temperature and other material parameters. The vaporization of the surface is assumed to be a continuous function of surface temperature.

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