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Published September 25, 2018 | public
Journal Article

Importance of the nozzle-exit boundary-layer state in subsonic turbulent jets

Abstract

To investigate the effects of the nozzle-exit conditions on jet flow and sound fields, large-eddy simulations of an isothermal Mach 0.9 jet issued from a convergent-straight nozzle are performed at a diameter-based Reynolds number of 1 x 10^6. The simulations feature near-wall adaptive mesh refinement, synthetic turbulence and wall modelling inside the nozzle. This leads to fully turbulent nozzle-exit boundary layers and results in significant improvements for the flow field and sound predictions compared with those obtained from the typical approach based on laminar flow in the nozzle. The far-field pressure spectra for the turbulent jet match companion experimental measurements, which use a boundary-layer trip to ensure a turbulent nozzle-exit boundary layer to within 0.5 dB for all relevant angles and frequencies. By contrast, the initially laminar jet results in greater high-frequency noise. For both initially laminar and turbulent jets, decomposition of the radiated noise into azimuthal Fourier modes is performed, and the results show similar azimuthal characteristics for the two jets. The axisymmetric mode is the dominant source of sound at the peak radiation angles and frequencies. The first three azimuthal modes recover more than 97 % of the total acoustic energy at these angles and more than 65 % (i.e. error less than 2 dB) for all angles. For the main azimuthal modes, linear stability analysis of the near-nozzle mean-velocity profiles is conducted in both jets. The analysis suggests that the differences in radiated noise between the initially laminar and turbulent jets are related to the differences in growth rate of the Kelvin–Helmholtz mode in the near-nozzle region.

Additional Information

© 2018 Cambridge University Press. (Received 15 September 2017; revised 7 March 2018; accepted 4 June 2018) The LES studies were supported by NAVAIR SBIR project under the supervision of J. T. Spyropoulos, with computational resources provided by DoD HPCMP at the ERDC DSRC supercomputer facility. G.A.B. would like to thank the main architects of the Charles solver, F. Ham and S. T. Bose, for their contributions to the LES studies. P.J. acknowledges the support of the French National Research Agency (ANR) through the project COOLJAZZ. Part of this work was performed during the Center for Turbulence Research Summer Program 2014 at Stanford University. The authors also thank S. Piantanida for performing the experimental measurements reported in figures 17 and 26.

Additional details

Created:
August 19, 2023
Modified:
October 18, 2023