2 edition of **Numerical simulation of free shear flows** found in the catalog.

Numerical simulation of free shear flows

- 249 Want to read
- 25 Currently reading

Published
**1993**
by National Aeronautics and Space Administration, National Technical Information Service, distributor in [Washington, DC], [Springfield, Va
.

Written in English

- Shear flow -- Computer simulation.

**Edition Notes**

Other titles | Towards a predictive computational aeroacoustics capability. |

Statement | W.Y. Soh. |

Series | NASA contractor report -- 19105., NASA contractor report -- NASA CR-19105. |

Contributions | United States. National Aeronautics and Space Administration. |

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

Format | Microform |

Pagination | 1 v. |

ID Numbers | |

Open Library | OL14695925M |

Many important phenomena in fluid motion are evident in vortex flow, i.e., flows in which vortical structures are significant in determining the whole flow. This book, which consists of lectures given at a NATO ARW held in Grenoble (France) in June , provides an up-to-date account of. The aim of this paper is to investigate the influence of different turbulence models (k−ε, RNG k−ε, and SST k−ω) on the numerical simulation of cavitating flow in thermosensitive fluid. The filter-based model and density correction method were employed to correct the turbulent viscosity of the three turbulence models.

Free shear flows, like those of mixing layers, are encountered in aerodynamics, in the atmosphere, and in the ocean as well as in many industrial applications such as flow reactors or combustion chambers. It is, therefore, crucial to understand the mechanisms governing the process of transition to turbulence in order to predict and control the evolution of the flow. A numerical study was made of flow behind a circular cylinder in a uniform flow, where the cylinder was rotationally oscillated in time. The temporal behavior of vortex formation was scrutinized over broad ranges of the two externally specified parameters, i.e., the dimensionless rotary oscillating frequency (⩽S f ⩽) and the maximum angular amplitude of .

Hwang RR, Sue YC () Numerical simulation of shear effect on vortex shedding behind a square cylinder. Int J Numer Meth Fluids – CrossRef zbMATH Google Scholar Kalita JC, Ray RK () A transformation-free hoc scheme for incompressible viscous flows past an impulsively started circular cylinder. This review describes some of the important developments in the numerical investigation of transition to turbulence in wall-bounded and free shear flows during the past decade. The evolution of numerical techniques and models as well as the advances in our theoretical understanding of the physics of laminar-turbulent transition that were achieved using these .

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Free Shear Layer. Free shear layers are more sensitive to small freestream values of ω∞ and larger values of ω are needed in the freestream. From: Analysis of Turbulent Flows with Computer Programs (Third Edition), Related terms: Turbulence; Boundary Layer; Direct Numerical Simulation; Eddy Viscosity; Reynolds' Number; Velocity.

Journals & Books; Help Download full Export. Advanced. Journal of Non-Newtonian Fluid Mechanics. Vol Issue 3, JunePages Numerical simulation of non-newtonian free shear flows at high reynolds numbers. Author links open overlay panel J. Azaiez G.M. Homsy 1. Show more. https: Free shear flow.

Mixing layer. Non Cited by: A numerical study of turbulent supersonic isothermal-wall channel flow 26 April | Journal of Fluid Mechanics, Vol.

Compressibility effects and mixing enhancement in turbulent free shear flows. Direct numerical simulations of turbulent free shear flows have been shown to be in generally good agreement with self.-similarity theory and laboratory data. The temporal development of a number of important statistical quantities has been shown to have the proper behavior, and the spatial evolution of the flow field is consistent with Cited by: 7.

DIRECT NUMERICAL SIMULATION OF FREE-SURFACE AND INTERFACIAL FLOW. Annual Review of Fluid Mechanics Figure 4: Configuration of a lamellar fluid when a shear flow is applied. The shear velocities are v = 0 (a), v = (b), and v = (c) (Gonnella et al ).Cited by: Compressibility, Turbulence and High Speed Flow introduces the reader to the field of compressible turbulence and compressible turbulent flows across a broad speed range, through a unique complimentary treatment of both the theoretical foundations and the measurement and analysis tools currently used.

The book provides the reader with the necessary background. GPU accelerated flow solver for direct numerical simulation of turbulent flows. which is the flow deriving from the turbulent mixing of two streams with different velocities.

Such flow is a prototype free shear layer, frequently encountered in a number of engineering applications (e.g. supersonic ejectors, scramjet engines), and it is also. This book is a great reference for basic concepts regarding turbulent flows as well as numerical simulations of turbulence, i.e.

Reynolds-Averaged Navier-Stokes (RANS) modeling, Large Eddy Simulation (LES), and Direct Numerical Simulation (DNS). Part I of the book deals with some of the fundamentals of turbulence: the statistical approach to Reviews: Simulations of turbulent shear flows by direct numerical solution of the three-dimensional Navier-Stokes equations are reported.

The momentumless wake of a self-propelled body is simulated, and equations are presented describing free-slip and no-slip boundary conditions as well as the initial conditions. The axial variation of the maximum turbulent intensity and the.

Large eddy simulation (LES) explicitly calculates the large-scale vortex field and parameterizes the small-scale vortices. In this study, LES and κ-ε models were developed for a specific geometrical configuration of backward-facing step (BFS).

The simulation results were validated with particle image velocimetry (PIV) measurements and direct numerical simulation. Numerical Simulation of Turbulent Flows. Annual Review of Fluid Mechanics Figure 4: Configuration of a lamellar fluid when a shear flow is applied.

The shear velocities are v = 0 (a), v = (b), and v = (c) (Gonnella et al ). Figure 9: Simulation of plate in free fall carried out by using a cut-cell method (Mittal et al. Preface; Nomenclature; Part I. Fundamentals: 1. Introduction; 2. The equations of fluid motion; 3. Statistical description of turbulence; 4.

Mean flow equations; 5. Direct Numerical Simulation of Controlled Shear Flows 13 Fig. 13 Wall temperature for steady blo wing through four rows of holes into a radiation-adiabatic ﬂat-plate boundary layer at.

This contribution is concerned with the simulation of turbulent shear flows. First, direct numerical simulations (DNS) are introduced, focusing on the challenges associated with computing turbulent flows without any empirical modelling.

The numerical method of one of our DNS codes is presented in detail and its performance on different HPC. Numerical Simulations of Flows with Moving Contact Lines. Figure 4: Configuration of a lamellar fluid when a shear flow is applied.

The shear velocities are v = 0 (a), v = (b), and v = (c) (Gonnella et al ). Figure 9: Simulation of plate in free fall carried out by using a cut-cell method (Mittal et al.

These plots. Direct numerical simulation (DNS) and large-eddy simulation (LES) are carried out to investigate the frequency effect of zero-net-mass-flux forcing (synthetic jet) on a generic separated flow. Free Shear Flows Javier Jimenez´ School of Aeronautics Universidad Politecnica de Madrid´ Summary This chapter and the next one describe particular classes of turbulent ﬂows.

The present one deals with incompressible constant-density ﬂows away from walls, which include shear layers, jets and wakes behind bodies. It can be divided into two. Two examples of controlled boundary-layer flows are discussed to illustrate the potential of advanced shear-flow control for drag or heat-load reduction.

Delay of the drag-increasing laminar-turbulent transition, a procedure generally termed laminar flow control (LFC), is demonstrated in a three-dimensional boundary-layer as present on a swept.

Purchase Numerical Simulation of Non-Newtonian Flow, Volume 1 - 1st Edition. Print Book & E-Book. ISBNWith the advent of super computers during the last ten years, the numerical simulation of viscous fluid flows modeled by the Navier-Stokes equations is becoming a most useful tool in Aircraft and Engine Design.

In fact, compressible Navier-Stokes solvers tend to constitute the basic tools for many. Numerical simulation of inelastic frictional spheres in simple shear flow - Volume - C.

K. K. Lun, A. A. Bent.Get this from a library! Numerical simulation of free shear flows: towards a predictive computational aeroacoustics capability. [United States. National Aeronautics and Space Administration.;].Accurate numerical simulations of turbulent free shear flows were performed in order to study the behavior of certain critical turbulence quantities which have been difficult to measure in the laboratory.

The three-dimensional time-dependent nonlinear Navier-Stokes equations are solved by the direct numerical simulation technique without turbulence modeling or ad hoc closure .