Thermal/Flow, Electronic Systems Cooling, and Space Systems Thermal > Solution options
Parallel flow solver schemes
The following schemes are available for the parallel flow solver.
Fractional Step
Solves mass and momentum equations separately once per timestep or steady state iteration.
Fully Coupled Pressure-Velocity
Solves mass and momentum equations simultaneously for each timestep or steady state iteration. For each timestep or steady state iteration, the solver iterates on the pressure and velocity solution until convergence is achieved.
Recommended use cases for Fractional Step
The factional step scheme is usually faster than the fully coupled scheme. It saves you time when you work on long transient problems under the following conditions:
The density variation is insignificant: Δρ/ρ0 << 1 where ρ0 is a scale of the density field and Δρ is the variation of density for the problem.
The timestep required to resolve the transient behavior to the desired accuracy is sufficiently small to imply a CFL number < 10. In this case, you require the same timestep size for both schemes. But, because the fractional step scheme is less computationally expensive on a per-timestep basis, it is faster than the fully coupled scheme. This is typically true of bluff body aerodynamics problems, for example, where you want to capture vortex shedding. In cases where the velocity field is not inherently strongly transient, but where the unsteady behavior is instead due to something like a time-varying heat load, it is often possible to obtain accurate results with the fully coupled scheme using a much larger timestep than with the fractional step scheme. Because the fully coupled scheme is generally more robust, and may even be computationally less expensive due to its ability to resolve the problems with a coarser timestep, for this class of problems, use the fully coupled scheme.
Note:
The following classes of problems are not supported by the fractional step scheme:
High speed flows
Models with rotational periodicity
Flap and bursting membrane
Recommended use cases for Fully Coupled Pressure-Velocity
For the following classes of problems, the fully coupled scheme is a better choice than the fractional step scheme:
Steady state problems
The fractional step scheme generally requires a smaller timestep size to reach convergence and is less stable. In some instances, the fractional step scheme appears to converge to a steady pressure field that is demonstrably incorrect when you use a timestep that is too large. Reducing the timestep sufficiently eliminates CFL warning messages.
Models with rotational frames of reference
Because the momentum equations are solved in a segregated manner with the fractional step scheme, the flow solver treats the Coriolis acceleration fully explicitly. Unless the rotation rate is very small or the Reynolds number is very low, you require a timestep consistent with a CFL number less than unity to avoid divergence or blowup.
Models with porous blockages
The fractional step scheme gives reasonable flow field results in the near-interface region only when the blockage resistance coefficients are quite low.
How do I
Define Advanced Parameters
Define Generic Entities
Learn more
Solution options
Understanding thermostat options for steady state analyses
Thermal initial conditions
3D flow initial conditions
Understanding ambient conditions
Joining fluid meshes
Understanding the turbulence models
Understanding out-of-bound options for time-dependent tables
Setting turbulence scale values
Turbulence Characteristics
Including additional input files for thermal analysis
Restarting a solution
Understanding time-varying time step
Target Temperature and Target Temperature Change
Solving the model
Look up more details
LES — Large Eddy Simulation
Adaptive time stepping method
Computed quantities for multiple convective BCs
Quick links
Command reference
Pre/Post video examples
Bulk Entry Descriptions
Simcenter 3D tutorials
Browse Simcenter 3D help by product area
Simcenter 3D Thermal/Flow, Electronic Systems Cooling, and Space Systems Thermal boundary conditions
Parallel flow solver schemes, Simcenter 3D 2021.1 Series
© 2020 Siemens
window.mainLanguage="en_US"
window.delivId=""
window.projectId=""
MathJax.Hub.Config({ TeX: { extensions: ["autoload-all.js"] }, tex2jax: { displayMath: [ ] }, "SVG": { scale: 125 } });
Source: https://docs.sw.siemens.com/en-US/doc/289054037/PL20200601120302950.advanced/xid1218317 · retrieved 2026-07-17