What Can the Acoustics Module Do?
The Acoustics Module is a collection of physics interfaces for COMSOL Multiphysics adapted to a broad category of acoustics simulations in fluids and solids. This module is useful even if you are not familiar with computational techniques. It can serve equally well as an excellent tool for educational purposes.
The Acoustics Module also includes many specialized formulations and material models that can be used for dedicated application areas like thermoviscous acoustics used in miniature transducers and mobile devices or Biot’s equations for modeling poroelastic waves. It also includes many predefined couplings between physics, called Multiphysics couplings, to model, for example, vibroacoustic problems.
The module supports time-harmonic (frequency domain), eigenfrequency, modal, and transient studies for all fluids (depending on the acoustic equations solved) as well as static, transient, eigenfrequency, modal, and frequency-response for the analyses of wave propagation in structures.
The multiphysics environment is further extended as the module combines several dedicated numerical methods, including the finite element method (FEM), the boundary element method (BEM), ray tracing, and the discontinuous Galerkin finite elements method (dG-FEM).
The available physics interfaces include the following functionality:
•
Pressure acoustics: model the propagation of sound waves (pressure waves) in the frequency domain solving the Helmholtz equation or in the time domain solving the scalar wave equation. Pressure acoustics comes in different flavors depending on the numerical formulation used. This includes finite element (FEM) based interfaces for frequency and transient models, a boundary element (BEM) based interface only used in the frequency domain, and a discontinuous Galerkin (dG-FEM) formulation based interface used for transient simulations. The Acoustics Module has built-in couplings between BEM and FEM that allows for modeling hybrid FEM-BEM problems.
•
Acoustic-structure interaction: combine pressure waves in the fluid with elastic waves in the solid. The physics interfaces provide predefined multiphysics couplings at the fluid-solid interface.
•
Boundary mode acoustics: find propagating and evanescent modes in ducts and waveguides.
•
Thermoviscous acoustics: model the detailed propagation of sound in geometries with small length scales. This is acoustics including thermal and viscous losses explicitly. Also known as visco-thermal acoustics, thermo acoustics, or linearized compressible Navier-Stokes. In the time domain nonlinear effects can be included.
•
Aeroacoustics: model the influence a background mean flow has on the propagation of sound waves in the flow, so-called, flow borne noise/sound. Interfaces exist to solve the linearized potential flow, the linearized Euler equations, and the linearized Navier-Stokes equations in both time and frequency domain.
•
Compressible potential flow: determine the flow of a compressible, irrotational, and inviscid fluid.
•
Solid mechanics and elastic waves: solve structural mechanics problems and the propagation of elastic waves in solids.
•
Piezoelectricity: model the behavior of piezoelectric materials in a multiphysics environment solving for the electric field and the coupling to the solid structure.
•
Poroelastic waves: in porous materials model the coupled propagation of elastic waves in the solid porous matrix and the pressure waves in the saturation fluid. Biot’s equations are solved here. Includes options to include both thermal and viscous losses.
•
Ultrasound: in ultrasound problems transient propagation is important and it is also important to be able to solve models with many wavelengths. These interfaces are based in the discontinuous Galerkin or dG-FEM formulation.
•
Acoustic diffusion equation: solve a diffusion equation for the acoustic energy density distribution for systems of coupled rooms in room acoustic applications.
•
Ray acoustics: compute trajectories and intensity of acoustic rays in room acoustic as well as underwater acoustic applications. Determine the impulse response with dedicated features in postprocessing.
•
Pipe acoustics: use this physics interface to model the propagation of sound waves in pipe systems including the elastic properties of the pipe. The equations are formulated in 1D for fast computation and can include a stationary background flow.
All the physics interfaces include a large number of boundary conditions. For the pressure acoustics applications, you can choose to analyze the scattered wave in addition to the total wave. Impedance conditions can be used to mimic a specific acoustic behavior at a boundary, for example, the acoustic properties of the human ear or a mechanical system approximated by a simple RCL circuit. Perfectly matched layers (PMLs) and absorbing layers provide accurate simulations of open pipes and other models with unbounded domains. The modeling domain includes support for several types of damping and losses that occur in porous materials (poroacoustics) or that are due to viscous and thermal losses (narrow region acoustics). For results evaluation of pressure acoustics models, you can compute the exterior acoustic field (phase and magnitude) and plot it in predefined radiation pattern plots.