The Impedance condition adds a boundary condition with the option to select between several built-in impedance models that allow modeling frequency dependent impedance conditions in the time domain. The impedance condition defines a relation between the local total acoustic pressure
pt and the normal acoustic velocity
n⋅ut, that is, the (normal) specific acoustic impedance
Zn (SI unit Pa·s/m). The condition specifies the normal velocity
The Impedance boundary condition is a good approximation of a locally reacting surface — a surface for which the normal velocity at any point depends only on the pressure at that exact point. This condition can be used to model the properties of artificial boundaries like a wall treatment in room acoustics. When the impedance is set equal to the characteristic specific impedance of a propagating plane wave
ρc, the condition represents the simplest nonreflecting boundary condition. This is also the default value of the impedance when the condition is added.
Select the Impedance model as
User defined (resistive) (the default),
Serial coupling RCL, or
General local reacting (rational approximation). The different options are as follows:
For the User defined (resistive) option represents a purely resistive constant impedance. The values entered here can only be real valued and constant in time.
Enter a value or expression for the Specific impedance Zn (SI unit: Pa·s/m). The default expression is
pate.c*pate.rho which is the characteristic specific impedance
ρc of a propagating plane wave.
The Serial coupling RCL option defines a simple spring-mass-damper system in the form of a serially coupled RCL circuit. This option can be used to approximate many systems that exhibit a simple damped resonant characteristic. The RCL condition will exhibit a simple frequency dependent behavior.
The General local reacting (rational approximation) option offers the most general and flexible form for defining a frequency dependent impedance condition in the time domain. The condition relies on a rational approximation (or rational expansion) of the frequency dependent admittance
Y(
f). This approximation has an analytical inverse Fourier transform and can thus be used to define the same frequency dependency in the time domain, by setting up a system of memory ODEs. These ODEs are automatically defined by the feature and solved on the impedance boundary. Approximating the frequency dependent admittance data can be performed by using the built-in
Partial Fraction Fit function.