fluent.com home page

   
 

What’s New in FLUENT 6.1

 

By Nicole M. Diana, FLUENT Product Market Manager

Multiphase flow
Dynamic mesh
Rotating equipment
Reacting flow
Heat transfer and phase change
Other enhancements

The release of FLUENT 6.1 is planned for the beginning of 2003. This version is packed with many exciting new features and capabilities in several focus areas, such as multiphase flow, dynamic mesh, rotating equipment, reacting flow, and heat transfer and phase change. The release is the result of a planning, development, and testing process in which specific industrial applications are targeted for each new feature release. Clients are interviewed to identify requirements and provide relevant test cases. The targeted applications are subjected to a matrix of industrial-strength test cases and three levels of progressively simpler cases. The industrial-strength test cases must be passed in order for the targeted functionality to be included in a release. Target applications for FLUENT 6.1 include: bubble column reactors, fluidized bed reactors, packed bed reactors, surface reactions in CVD reactors, in-cylinder flows, store separation and missile launch, turbomachinery, underhood flows, and fuel injector pumps. Some of the highlights of the new functionality are presented below.

View Larger Image
Liquid volume fraction in a boiling simulation in which a column of water is exposed to a heat source at the center of its base

Multiphase flow

The Eulerian multiphase model has been extended to allow for heat and mass transfer. Mass transfer can also be included with VOF simulations. The mixture model can now handle compressibility in one phase, and several standard drag laws have been added. The discrete phase spray models can now be used for transient as well as steady-state analysis, and particles can interact with both moving and sliding zones. A new spray/wall impingement model has been implemented that allows for tangential droplet motion that can arise from spray-wall interaction.

Dynamic mesh

Offered as a beta capability in FLUENT 6.0, the dynamic mesh model will be officially released in FLUENT 6.1, with parallel functionality fully supported. The novel approach used by this model requires the user to specify only the initial mesh and boundary conditions for the moving wall(s). The solver automatically generates all subsequent changes in the mesh with each time step, using one or more of three available algorithms. (See the article on page 5 for more details.)


Deposition of gallium arsenide in a vertical rotating disc reactor
Courtesy of EMCORE Corp.

Rotating equipment

For turbomachinery and rotating equipment simulations, a sliding mesh preview tool has been provided to help determine if the mesh is valid prior to launching a calculation. A mass flow outlet is now available, and an enthalpy conservation option has been added to the mixing plane model. For modeling real gases, a custom real gas model can be specified through a user-defined function, and a template for the Redlich-Kwong equation of state is also available. Turbomachineryspecific post-processing tools have been expanded to address multistage problems.

View Larger Image
Contours of vapor volume fraction for a 2D hydrofoil with Cavitation Number 0.91
View Larger Image
Comparison of computed (blue line) and experimental (red circles) pressure variation on the suction side of the 2D hydrofoil shown above
View Larger Image
View factor calculation time (min) for a typical automotive underhood simulation illustrates the surface-to-surface radiation model enhancements in FLUENT 6.1

Reacting flow

For simulations involving surface reactions, site species and bulk species are now distinguished from one another, allowing for multi-step surface reactions with deposition and etching.

The porous media model has also been enhanced to better handle chemically reacting flows, typical of packed bed reactors. The actual physical (interstitial) velocities in porous media are now computed in addition to the superficial velocities, to better account for the effects of fluid acceleration. Chemical reactions can be limited to individual zones and can be disabled in certain zones, if desired. This is helpful for modeling a reactor that contains a catalyst region. Surface reactions can also now be specified on walls adjacent to porous zones.

Also new is the composition PDF transport model, implemented through a collaboration with Professor Stephen Pope of Cornell. It provides an accurate turbulence-chemistry interaction model for real finite-rate chemistry in turbulent flames.

Heat transfer and phase change

A partial enclosure option has been added to the surface-to-surface radiation model that allows portions of the geometry that are not important for the radiative exchange calculation to be ignored. In addition, the view factor solver has been upgraded to a new version of Chaparral. These two improvements significantly reduce the CPU and memory requirements for the view-factor calculation. A new, robust cavitation model that can handle highly cavitating flows has been added that accurately predicts the pressure profile, even for very high pressure conditions. A new heat exchanger model has also been implemented.

Other enhancements

There are several solver-related enhancements. A new gradient calculation scheme can be selected that may result in more accurate predictions on all meshes, but particularly on unstructured meshes. Other new features include fully automatic mesh refinement, the ability to run DPM simulations on distributed memory systems, and the ability to read cases with non-conformal and sliding interfaces directly into the parallel solver without encapsulation.

The new detached eddy simulation (DES) model, which uses LES in the core turbulent region and RANS in the wall-dominated region, is a practical alternative to LES simulations for high Reynolds number external aerodynamic flows, since it is able to capture the physics in an affordable manner. The V2F model from Cascade Technologies is now embedded and available for an additional fee. This four-equation turbulence model is well-suited for low Re number flows.

Additional new features in FLUENT 6.1 include the ability to couple the WAVE engine simulation code with FLUENT, a built-in capability to compute discrete Fourier transforms of time series data, and the ability to automatically build compiled UDF libraries at the push of a button. In addition to the UDF-based acoustics module that was released in July, FLUENT 6.1 includes two other UDF-based add-on modules: a magnetohydrodynamics model and a continuous fiber model. All three modules will be included on the FLUENT 6.1 CDs. License keys will be needed to access the magnetohydrodynamics and continuous fiber modules; contact your local Fluent office for more details.

This is only a sampling of the capabilities that will be delivered in FLUENT 6.1. For more details, review the release notes that are posted on the User Services Center. At Fluent, we are all very excited about the expanding range of applications that can be addressed with the FLUENT 6 platform.


Previous Article FluentNEWS Next Article