The Goldstein model allows you to compute the local
acoustic power of quadrupole-generated noise (generated per unit volume) for anisotropic
turbulent flows in axisymmetric jets.
Note | This model only solves for noise sources—not for acoustic
wave propagation. |
Table 1. Goldstein Model Reference
Theory
|
See Goldstein Axisymmetric Noise Source Model. |
Provided By
|
|
Example Node Path
|
|
Requires
|
- Space:
Axisymmetric
- Time: Steady or
Implicit Unsteady
- Material:
any but solid
- Flow: any
- Viscous
Regime: Turbulent
- Turbulence:
Reynolds-Averaged Navier-Stokes
- Reynolds-Averaged Turbulence: any
- Optional Models:
Aeroacoustics
- Aeroacoustics
Models: Broadband Noise
Sources
|
Properties
|
Key
properties are:
- Far-Field
Density
- Far-Field Sound
Speed
- Reference
Acoustic Power
See Goldstein Model Properties. |
Activates |
Field Functions
|
- Goldstein
Acoustic Power
- Goldstein
Acoustic Power DB
- Mesh Frequency Cutoff
Hz
See Field Functions. |
Goldstein Model Properties
- Far-Field Density
- The fluid density in the
far-field,
in Eqn. (4668).
- Far-Field Sound Speed
- The speed of sound in the far-field,
in Eqn. (4668).
- Reference Acoustic
Power
- The reference acoustic power
in the calculation of the acoustic power per
unit volume in dB, see Eqn. (4677).
Field Functions
- Goldstein Acoustic Power
- The local acoustic power per
unit volume in W/m3, see
given by Eqn. (4667).
- Goldstein Acoustic Power DB
- The local acoustic power per unit volume in
dB, see
given by Eqn. (4677).
- Mesh Frequency Cutoff Hz
- The frequency that the mesh can resolve in
Hz. For more information, see Qualifying the Mesh for the Desired Sound Frequency.