- Introduction
- COMSOL Multiphysics
- AC/DC Module
- Acoustics Module
- Batteries and Fuel Cells Module
- CAD Import Module and LiveLink™ Products
- CFD Module
- Chemical Reaction Engineering Module
- Electrodeposition Module
- Geomechanics Module
- Heat Transfer Module
- MEMS Module
- Microfluidics Module
- Plasma Module
- RF Module
- Structural Mechanics Module
- Subsurface Flow Module
- LiveLink™ for MATLAB®
- The COMSOL API
New Functionality in Version 4.2
New Physics Interfaces
- High Mach Number Flow interface for laminar and turbulent flow, handling flows with compressibility effects.
- Reacting Flow, Diluted Species multiphysics interface combining single-phase flow with mass transport of diluted species.
- Reacting Flow, Concentrated Species multiphysics interface combining single-phase flow with mass transport of concentrated species.
Single-Phase Flow
- Improved stabilization for the single-phase flow interfaces.
Multiphase Flow
- New Two-Phase Darcy’s Law interface for modeling of two-phase flow in porous media.
- New initialization for two-phase flow interfaces using a wall distance function.
- Improved stabilization for the Brinkman Equations and Free and Porous Media Flow interfaces.
Non-Isothermal Flow
- Thermal wall functions with turbulence now support the Surface-to-Surface Radiation, Reradiating Surface, and Highly Conductive Layer heat transfer boundary conditions.
- Vacuum pump boundary condition.
Porous Media Flow
- New multiphase flow in porous media interface that defines two sets of Darcy equations for the separate phases in porous media.
Fluid-Structure Interaction
- Improved solver settings for the Fluid-Structure Interaction interface.
Backward Compatibility vs. Version 3.5a
k-ω Turbulence Model
The k-ω turbulence model physics interface is not yet implemented in version 4.2. It is planned to be reintroduced in a future version of the CFD Module.
Version 4.2 includes automatic translation of models built with the previous k-ω turbulence model. When opened, the full model, including initial values and boundary conditions, is converted to the k-ε turbulence model. Once opened, the model can also be also be changed to the Low-Reynolds k-e Turbulence Model interface. The latter physics interface present an excellent alternative for higher accuracy in models including confined flows.

