Goldstein Model Reference

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.

NoteThis 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 [physics continuum] > Models > Broadband Noise Source Models
Example Node Path Continua > Physics 1 > Models > Goldstein
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, ρ 0 in Eqn. (4668).
Far-Field Sound Speed
The speed of sound in the far-field, c 0 in Eqn. (4668).
Reference Acoustic Power
The reference acoustic power P r e f 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 G A P given by Eqn. (4667).
Goldstein Acoustic Power DB
The local acoustic power per unit volume in dB, see G A P ( d B ) 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.