The wave speed c in the pipe can be different from the speed of sound cs in an open space. It then depends on the elastic properties of the pipe structure. It is defined in Equation 3-17 in the Governing Equations section.
The wave speed can be evaluated as sqrt(1/patd.invc2) or sqrt(1/pafd.invc2) during the analysis and results stage.
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For Infinite pipe enter a Wave number k (SI unit: rad/m). The default expression is pafd.omega*(sqrt(pafd.invc2)). This end impedance models the infinite pipe using the full (nonlinear) dispersion relation. It is valid for all Mach numbers but requires the additional input of the wave number k.
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For Flanged pipe, circular enter an Inner radius a (SI unit: m). The default expression is pafd.dh/2. This end impedance models the radiation impedance of a circular pipe terminated in an infinite baffle. It is an exact analytical result valid for all frequencies and pipe radii. In the low frequency limit it reduces to the classical results:
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For Flanged pipe, rectangular enter an Inner width wi (SI unit: m). The default is 5 cm (0.005 m). Also enter an Inner height hi (SI unit: m). The default is 10 cm (0.01 m). This end impedance models the radiation impedance of a pipe of rectangular cross section terminated in an infinite baffle. The model is only valid in the low frequency range where and .
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For Unflanged pipe, circular (low ka limit) or Unflanged pipe, circular enter an Inner radius a (SI unit: m). The default expression is pafd.dh/2. These two end impedance models prescribe the radiation impedance of an unflanged circular pipe (a pipe ending in free open space). The first model is the classical low-frequency approximation valid for . While the second model extends the frequency range to ka < 3.83.
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For User defined enter an End impedance Zend (SI unit: Pa⋅s/m). The default expression is pafd.rho*(sqrt(1/pafd.invc2)), which is ρ·c.
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