[1] B. Van Leer, Towards the ultimate conservative difference scheme, Ⅱ. Monotonicity andconservation combined in a second order scheme, J. Comp. Phys., 14 (1974), 361-370. [2] P. L. Roe, Numerical algorithms for the linear wave equation, Royal AircraftEstablishment Technical Report 81047 (1981). [3] P. L. Roe, Some contributions to the modelling of discontinuous flows. in ProceedingsAMS-SLAM Sum, on Large-Scale Comp. in Fluid Mech., 1983, edited by B. E. Engquistet al., Lectures in Appl. Math., 22, 2 (1985), 673. [4] S. R. Chakravarthy and S. Osher, High resolution applications of the Oshcr upwindscheme for the Euler equations, AIAA paper presented at 6th CFD Conference (1983). [5] P. K. Sweby, High resolution schemes using flux limiters for hyperbolic conservationlaws, SIAM J. Numer. Anal., 21, 5 (1984), 995-1011. [6] A. Harten, High resolution schemes for hyperbolic conservation laws, J. Comput. Phys.,49 (1983), 357-393. [7] A. Jameson, Positive schemes and shock modelling for compressible flows, Internat. J.for Numer. Methods Fluids, 20 (1995), 743-770. [8] Liu Ruxun, The study of the remainder effects of FDS, J. Comput. Phys. 9, 4 (1992),479. (in Chinese). [9] Liu Ruxun, The remainder-effect analysis of FDS and the applications to reforming oroptimazing of FDS, J. of CUST, 24, 3 (1994), 271. (in Chinese). [10] Liu Ruxun and Zhou Zhaohui, The remainder-effect analysis of FDS and theapplications, Applied Mathematics and Mechanics (English Ed.). 16, 1 (1995). 87-96. |