[1] LAX P, WENDROFF B. Systems of conservation laws[J].Comm Pure Appl Math,1960,13:217-237. [2] VAN LEER B. Towards the ultimate conservative difference scheme V:A second order sequel to Godunov's method[J]. J Comput Phys,1979,32:101-136. [3] HARTEN A. High resolution schemes for hyperbolic conservation laws[J]. J Comput Phys, 1983,49:357-393. [4] HARTEN A, ENGQUIST B, OSHER S. Uniformly high order accurate essentially non-oscillatory schemes, Ⅲ[J]. J Comput Phys, 1987,71:231-303. [5] SHU C W, OSHER S. Efficient implementation of essentially non-oscillatory shock capturing schemes[J]. J Comput Phys,1988, 77:439-471. [6] LIU X D, OSHER S, CHAN T. Weighted essentially non-oscillatory schemes[J]. J Comput Phys, 1994,115:200-12. [7] JIANG G S, SHU C W. Efficient implementation of weighted ENO schemes[J]. J Comput Phys,1996,126:202-28. [8] COCKBURN B, SHU C W. The Runge-Kutta discontinuous Galerkin method for conservation laws V:Multidimensional systems[J]. J Comput Phys, 1998,141:199-224. [9] HENRICK A K, ASLAM T D, Powers J M. Mapped weighted essentially non-oscillatory schemes:Achieving optimal order near critical points[J]. J Comput Phys,2005,207(2):542-567. [10] BORGES R, CARMONA M, COSTA B. An improved weighted essentially non-oscillatory scheme for hyperbolic conservation laws[J]. J Comput Phys, 2008, 227:191-211. [11] ZHAO F, PAN L, LI Z, WANG S. A new class of high-order weighted essentially non-oscillatory schemes for hyperbolic conservation laws[J]. Computers and Fluids, 2017, 159:81-94. [12] HARTEN A, CHAKRAVARTHY S R. Multidimensional ENO schemes for general geometries[R]. ICASE Report No.91-76, 1991. [13] ABGRALL R. On essentially non-oscillatory schemes on unstructured meshes:Analysis and implementation[J]. J Comput Phys, 1994,114:45-58. [14] SONAR T. On the construction of essentially non-oscillatory finite volume approximations to hyperbolic conservation laws on general triangulations:Polynomial recovery, accuracy and stencil selection[J]. Comput Methods Appl Mech Engrg, 1997, 140:157-181. [15] FRIEDRICH O. Weighted essentially non-oscillatory schemes for the interpolation of mean values on unstructured grids[J]. J Comput Phys,1998, 144:194-212. [16] DUMBSER M, KASER M. Arbitrary high order non-oscillatory finite volume schemes on unstructured meshes for linear hyperbolic systems[J]. J Comput Phys, 1998, 221:693-723. [17] HU C, SHU C W. Weighted essentially non-oscillatory schemes on triangular meshes[J]. J Comput Phys,1999,150:97-127. [18] SHI J, HU C, SHU C W. A technique of treating negative weights in WENO schemes[J]. J Comput Phys, 2002, 175:108-127. [19] LIU Y, ZHANG Y T. A robust reconstruction for unstructured WENO schemes[J]. J Sci Comput, 2013,54:603-621. [20] TORO E. Riemann solvers and numerical methods for fluid dynamics[M]. Springer, 1997. [21] WOODWARD P, COLELLA P. Numerical simulations of two-dimensional fluid flow with strong shocks[J]. J Comput Phys,1984,54:115-73. [22] WANG Q, REN Y, LI W. Compact high order finite volume method on unstructured grids Ⅱ:Extension to two-dimensional Euler equations[J]. J Comput Phys, 2016,314:883-908. |