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Published **1983**
by National Aeronautics and Space Administration, Langley Research Center in Hampton, Va .

Written in English

- Multiphase flow -- Mathematical models.,
- Fluid dynamics (Space environment) -- Mathematical models.

**Edition Notes**

Statement | M. Napolitano and A. Dadone. |

Series | NASA contractor report -- NASA CR-172264. |

Contributions | Dadone, A., Langley Research Center., Institute for Computer Applications in Science and Engineering. |

The Physical Object | |
---|---|

Format | Microform |

Pagination | 1 v. |

ID Numbers | |

Open Library | OL17557276M |

Cite this paper as: Fortunato B., Magi V. () An implicit Lambda method for 2-D viscous compressible flows. In: Deshpande S.M., Desai S.S., Narasimha R. (eds) Fourteenth International Conference on Numerical Methods in Fluid by: 6. A 'read' is counted each time someone views a publication summary (such as the title, abstract, and list of authors), clicks on a figure, or views or downloads the full-text. In numerical analysis, the Crank–Nicolson method is a finite difference method used for numerically solving the heat equation and similar partial differential equations. It is a second-order method in time. It is implicit in time and can be written as an implicit Runge–Kutta method, and it is numerically method was developed by John Crank and Phyllis Nicolson in the . Implicit-explicit (IMEX) schemes have been widely used, especially in conjunction with spectral methods, for the time integration of spatially discretized partial .

Fourteenth International Conference on Numerical Methods in Fluid Dynamics Proceedings of the Conference Held in Bangalore, India, 11–15 July Vortex methods for three-dimensional separated flows. An implicit Lambda method for 2-D . The IAEA 3-D PWR problem (Benchmark Problem Book, ) is a standard benchmark problem to measure the performance of neutronic calculation core is composed by fuel assemblies including 9 fully rodded fuel assemblies and 4 partially rodded fuel assemblies, as it is shown in Fig. reflector is modelled by means of 64 assemblies surrounding the : S. González-Pintor, D. Ginestar, G. Verdú. The main methods of this type which we shall consider are: Adams-Bashforth. These methods are explicit with methods of order k being k-step. Methods of order from one to three have the formulae. The first order method is more normally called the Euler method. Adams-Moulton. These methods are implicit with methods of order k being -step. In this paper, an implicit restarted Arnoldi method is presented as an advantageous alternative to classical methods as the Power Iteration method and the Subspace Iteration method.

@article{osti_, title = {A parallel domain decomposition-based implicit method for the Cahn–Hilliard–Cook phase-field equation in 3D}, author = {Zheng, Xiang and Yang, Chao and State Key Laboratory of Computer Science, Chinese Academy of Sciences, Beijing and Cai, Xiao-Chuan and Keyes, David and Department of Applied Physics. SIAM Journal on Numerical Analysis , Abstract | PDF ( KB) () Implicit-Explicit Formulations of a Three-Dimensional Nonhydrostatic Cited by: In numerical linear algebra, the Alternating Direction Implicit (ADI) method is an iterative method used to solve Sylvester matrix equations. It is a popular method for solving the large matrix equations that arise in systems theory and control, and can be formulated to construct solutions in a memory-efficient, factored form. It is also used to numerically solve parabolic and elliptic . The Two- and Three-Dimensional Navier-Stokes Equations [] Background []. The Navier-Stokes equations describe the motion of a fluid. In order to derive the Navier-Stokes equations we assume that a fluid is a continuum (not made of individual particles, but rather a continuous substance) and that mass and momentum are conserved.

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