Why Are Multiple Pressure-Velocity Coupling Algorithms Used in ANSYS Fluent?

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SUMMARY

Multiple pressure-velocity coupling algorithms in ANSYS Fluent, including SIMPLE, SIMPLEC, PISO, Fractional Step Method (FSM), and Coupled, are essential for optimizing fluid dynamics simulations. SIMPLEC is preferred for uncomplicated laminar flows due to its faster convergence, while PISO is recommended for transient flow calculations with larger time steps. The FSM, available with the NITA scheme, offers a computationally efficient alternative but may lack stability in certain applications. The Coupled solver provides robust performance for steady-state flows but is not compatible with specific boundary conditions.

PREREQUISITES
  • Understanding of fluid dynamics principles, particularly the Navier-Stokes equations.
  • Familiarity with ANSYS Fluent software and its solver options.
  • Knowledge of turbulence models, especially LES (Large Eddy Simulation).
  • Experience with computational fluid dynamics (CFD) simulations and their convergence criteria.
NEXT STEPS
  • Research the differences between SIMPLE and SIMPLEC algorithms in ANSYS Fluent.
  • Explore the implementation and advantages of the PISO algorithm for transient flow simulations.
  • Investigate the Non-Iterative Time Advancement (NITA) scheme and its impact on computational efficiency.
  • Learn about the Coupled solver's application in steady-state flow problems and its limitations.
USEFUL FOR

Fluid dynamics engineers, computational fluid dynamics (CFD) analysts, and researchers seeking to enhance simulation accuracy and efficiency in ANSYS Fluent.

humphreybogart
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In Fluent, there are several 'pressure-velocity coupling' algorithms.

Why are these necessary when, in many fluid mechanics textbooks, it is proposed that for incompressible fluids, an equation for Pressure can be found by taking the divergence of the Navier-Stokes equation, and inverting using the Biot-Savart law?
 
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ANSYS's documentation package describes in great detail the applications of each solver. It appears most of the reasons you would choose one solver over another relate to the kind of problem you're solving, and the FEA model's parameters.

See here: https://www.sharcnet.ca/Software/Fluent6/html/ug/node1021.htm

ANSYS Documentation (FLUENT 6.3) said:
SIMPLE vs. SIMPLEC
For relatively uncomplicated problems (laminar flows with no additional models activated) in which convergence is limited by the pressure-velocity coupling, you can often obtain a converged solution more quickly using SIMPLEC. With SIMPLEC, the pressure-correction under-relaxation factor is generally set to 1.0, which aids in convergence speed-up.

ANSYS Documentation (FLUENT 6.3) said:
PISO
(25.4.3) with neighbor correction is highly recommended for all transient flow calculations, especially when you want to use a large time step. (For problems that use the LES turbulence model, which usually requires small time steps, using PISO may result in increased computational expense, so SIMPLE or SIMPLEC should be considered instead.) PISO can maintain a stable calculation with a larger time step and an under-relaxation factor of 1.0 for both momentum and pressure. For steady-state problems, PISO with neighbor correction does not provide any noticeable advantage over SIMPLE or SIMPLEC with optimal under-relaxation factors.

ANSYS Documentation (FLUENT 6.3) said:
Fractional Step Method
25.4.3, is available when you choose to use the NITA scheme (i.e., the Non-Iterative Time Advancement option in the Solver panel). With the NITA scheme, the FSM is slightly less computationally expensive compared to the PISO algorithm. Whether you select FSM or PISO depends on the application. For some problems (e.g., simulations that use VOF), FSM could be less stable than PISO.

ANSYS Documentation (FLUENT 6.3) said:
Coupled
25.4.3. This solver offers some advantages over the pressure-based segregated algorithm. The pressure-based coupled algorithm obtains a more robust and efficient single phase implementation for steady-state flows. It is not available for cases using the Eulerian multiphase, NITA, and periodic mass-flow boundary conditions.
 

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