| Numerical solution of the Euler equations by finite volume methods using Runge Kutta time stepping schemes A Jameson, W Schmidt, E Turkel 14th fluid and plasma dynamics conference, 1259, 1981 | 6014 | 1981 |
| Radiation boundary conditions for wave‐like equations A Bayliss, E Turkel Communications on Pure and Applied Mathematics 33 (6), 707-725, 1981 | 1403 | 1981 |
| Preconditioned methods for solving the incompressible and low speed compressible equations E Turkel Journal of computational physics 72 (2), 277-298, 1987 | 1184 | 1987 |
| Boundary conditions for the numerical solution of elliptic equations in exterior regions A Bayliss, M Gunzburger, E Turkel SIAM Journal on Applied Mathematics 42 (2), 430-451, 1982 | 874 | 1982 |
| On central-difference and upwind schemes RC Swanson, E Turkel Journal of computational physics 101 (2), 292-306, 1992 | 658 | 1992 |
| Preconditioning techniques in computational fluid dynamics E Turkel Annual Review of Fluid Mechanics 31 (1), 385-416, 1999 | 559 | 1999 |
| Absorbing PML boundary layers for wave-like equations E Turkel, A Yefet Applied Numerical Mathematics 27 (4), 533-557, 1998 | 469 | 1998 |
| Review of preconditioning methods for fluid dynamics E Turkel Applied Numerical Mathematics 12 (1-3), 257-284, 1993 | 386 | 1993 |
| Implicit schemes and 𝐿𝑈 decompositions A Jameson, E Turkel Mathematics of Computation 37 (156), 385-397, 1981 | 384 | 1981 |
| Dissipative two-four methods for time-dependent problems D Gottlieb, E Turkel Mathematics of computation 30 (136), 703-723, 1976 | 349 | 1976 |
| An iterative method for the Helmholtz equation A Bayliss, CI Goldstein, E Turkel Journal of Computational Physics 49 (3), 443-457, 1983 | 329 | 1983 |
| Far field boundary conditions for compressible flows A Bayliss, E Turkel Journal of Computational Physics 48 (2), 182-199, 1982 | 328 | 1982 |
| On accuracy conditions for the numerical computation of waves A Bayliss, CI Goldstein, E Turkel Journal of Computational Physics 59 (3), 396-404, 1985 | 312 | 1985 |
| A fourth-order accurate finite-difference scheme for the computation of elastic waves A Bayliss, KE Jordan, BJ LeMesurier, E Turkel Bulletin of the Seismological Society of America 76 (4), 1115-1132, 1986 | 279 | 1986 |
| High-order finite difference methods for the Helmholtz equation I Singer, E Turkel Computer methods in applied mechanics and engineering 163 (1-4), 343-358, 1998 | 252 | 1998 |
| Artificial dissipation and central difference schemes for the Euler and Navier-Stokes equations R Swanson, E Turkel 8th Computational Fluid Dynamics Conference, 1107, 1987 | 247 | 1987 |
| Assessment of preconditioning methods for multidimensional aerodynamics E Turkel, R Radespiel, N Kroll Computers & Fluids 26 (6), 613-634, 1997 | 215 | 1997 |
| Compact 2D and 3D sixth order schemes for the Helmholtz equation with variable wave number E Turkel, D Gordon, R Gordon, S Tsynkov Journal of Computational Physics 232 (1), 272-287, 2013 | 180 | 2013 |
| Analytical and numerical studies of a finite element PML for the Helmholtz equation I Harari, M Slavutin, E Turkel Journal of Computational Acoustics 8 (01), 121-137, 2000 | 180 | 2000 |
| Accurate finite difference methods for time-harmonic wave propagation I Harari, E Turkel Journal of Computational Physics 119 (2), 252-270, 1995 | 171 | 1995 |
Matteo ParsaniKing Abdullah University of Science and TechnologyVerified email at kaust.edu.sa