By Ramon E Moore
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A. Trangenstein, and M. Welcome. Adaptive mesh reﬁnement on moving quadrilateral grids. In Proceedings of the 9th AIAA Computational Fluid Dynamics Conference, Buffalo, NY, June 1989. 13. V. Kuteev. Hydrogen pellet ablation and acceleration by current in high temperature plasmas. Nucl. Fusion, 35:431–453, 1995. 14. K. MacAulay. Two dimensional time dependent simulation of ablation of hydrogen pellets in hot magnetized fusion plasmas. PhD thesis, Princeton University, 1993. 15. A. K. MacAulay. Geometrical, kinetic and atomic physics effects in a two dimensional time dependent simulation of ablating fuel pellets.
3 Tracer Tomography To monitor the hazardous nonaqueous phase liquids (NAPLs), partitioning tracer tomography is an important subsurface imaging technique. The starting assumption is that there exists a steady ﬂow ﬁeld in form of a Darcy ﬂux, q(x) = −K(x)∇H(x). Each pumping test injects an impulse solution of partitioning tracers from a speciﬁc location xp into . The tracer concentration c(x, t) is then measured at a set of observation locations and for a set of time levels. 4) where θw and θn denote the saturation ﬁelds of water and NAPL, respectively.
Parks and M. Rosenbluth. Equilibrium pellet and liquid jet shape under high ablation pressures. Phys. Plasmas, 5:1380–1386, 1998. 22. P. J. Turnbull. Effect of transonic ﬂow in ablation cloud on lifetime of a solid hydrogen pellet in a plasma. Phys. Fluids, 21:1735–1741, 1978. 23. R. Reynolds, R. S. Woodward. A fully implicit numerical method for single-ﬂuid resistive magnetohydrodynamics. J. Comput. , 219:144–162, 2006. References 27 24. R. Samtaney, P. J. F. C. Jardin. An adaptive mesh semi-implicit conservative unsplit method for resistive MHD.
Computational functional analysis by Ramon E Moore