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Steven J. Massey Eagle Aeronautics, Inc. Alaa A. Elmiligui

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Presentation on theme: "Steven J. Massey Eagle Aeronautics, Inc. Alaa A. Elmiligui"— Presentation transcript:

1 Computational Analysis of a Chevron Nozzle Uniquely Tailored for Propulsion Airframe Aeroacoustics
Steven J. Massey Eagle Aeronautics, Inc. Alaa A. Elmiligui Analytical Services & Materials, Inc. Craig A. Hunter, Russell H. Thomas, S. Paul Pao NASA Langley Research Center and Vinod G. Mengle Boeing Company 12th AIAA/CEAS Aeroacoustics Conference Cambridge, MA May 8-10, 2006

2 Outline Motivation Objectives Numerical Tools
Review of Generic Jet-Pylon Effect Axi, bb, RR, RT Nozzle Configurations Analysis Procedure Results Chain from Noise to Geometry Summary Concluding Remarks NASA Langley Research Center May 8, 2006

3 General PAA Related Effects and Features On Typical Conventional Aircraft
Jet interaction with horizontal stabilizers Nacelle-airframe integration e.g. chines, flow distortion, relative angles Jet-pylon interaction of the PAA T-fan nozzle Pylon-slat cutout Jet influence on airframe sources: side edges Jet-flap trailing edge interaction Jet-flap impingement Jet and fan noise scattering from fuselage, wing, flap surfaces QTD2 partnership of Boeing, GE, Goodrich, NASA, and ANA NASA Langley Research Center May 8, 2006

4 Objectives To build a predictive capability to link geometry to noise for complex configurations To identify the flow and noise source mechanisms of the PAA T-Fan (quieter at take off than the reference chevron nozzle) NASA Langley Research Center May 8, 2006

5 Numerical Tools PAB3D Jet3D 3D RANS upwind code
Multi-block structured with general patching Parallel using MPI Mesh sequencing Two-equation k- turbulence models Several algebraic Reynolds stress models Jet3D Lighthill’s Acoustic Analogy in 3D Models the jet flow with a fictitious volume distribution of quadrupole sources radiating into a uniform ambient medium Uses RANS CFD as input Now implemented for structured and unstructured grids (ref AIAA ) NASA Langley Research Center May 8, 2006

6 Sample Grid Plane 31 Million Cells for 180o
PAB3D solution: 33 hours on 44 Columbia CPU’s (Itanium 2) Jet3D solution, 10 minutes on Mac NASA Langley Research Center May 8, 2006

7 Model Scale LSAF PAA Nozzles Analyzed
Four Nozzles Chosen for Analysis: Axisymmetric Nozzle (not an experimental nozzle) bb conventional nozzles RR state-of-the-art azimuthally uniform chevrons on core and fan RT PAA T-fan azimuthally varying chevrons on fan and uniform chevrons on core For more details see Mengle et al. AIAA NASA Langley Research Center May 8, 2006

8 Generic Pylon Effect Understanding - AIAA 05-3083
Core Flow Induced Off of Jet Axis by Coanda Effect Pairs of Large Scale Vortices Created TKE and Noise Sources Move Upstream Depending on Design Details can Result in Noise Reduction or Increase with Pylon Refs: AIAA , , , , , NASA Langley Research Center May 8, 2006

9 Analysis Procedure Start with established facts and work from derived to fundamental quantities to form connections to geometry Measured noise data (LSAF) SPL predictions (Jet3D) OASPL noise source histogram (Jet3D) Mass averaged, non-dimensional turbulence intensity (PAB3D) OASPL noise source maps (Jet3D) Turbulence kinetic energy (PAB3D) Axial vorticity Cross flow streamlines Vertical velocity Total temperature Total temperature centroid Geometry NASA Langley Research Center May 8, 2006

10 Jet3D SPL Predictions with LSAF
bb predicted within 1 dB for whole range RR over predicted by 1 dB for frequencies < 10 kHz, under predicted by up to 2 dB for high frequencies RT predicted within 1 dB for whole range, under predicted high frequencies Tunnel noise * Trends predicted correctly increasing confidence of flow and noise source linkage * Axi case not thrust matched to others Observer located on a 68.1D radius from the fan nozzle exit at an inlet angle of 88.5 deg. and an azimuthal angle of 180 deg. LSAF data from Mengle et al. AIAA 2006–2467 NASA Langley Research Center May 8, 2006

11 Noise Prediction – CFD Link
Jet3D OASPL Histogram PAB3D: Mass-Avg TKE Noise and TKE sources relative to Axi are consistent with previous pylon understanding of mixing Mass-Avg TKE qualitatively matches noise source histogram bb, RR, RT intersect near x/D = 10 Axi crosses bb, RR at x/D = 12 Axi crosses RT at x/D = 12.75 NASA Langley Research Center May 8, 2006

12 LAA – CFD Correspondence
Axi bb RR RT Peak noise sources correspond with peak TKE Local noise increased by chevron length Cross flow stream lines show shear layer vorticity orientation NASA Langley Research Center May 8, 2006

13 Beginning Fan/Core Shear Merger
Axi bb RR RT Noise and TKE peak as layers merge RR levels slightly lower than bb RT merger delayed, much lower levels Axi noise asymmetry due to LAA observer location. TKE is symmetric Axial velocity 20 times stronger than cross flow, thus strongest vortex would take about 60D for one revolution NASA Langley Research Center May 8, 2006

14 Peak Noise From Shear Merger
Axi bb RR RT bb, RR peak shown; RT peaks 0.5D later, one contour lower than bb and RR Unmerged Axi with lower noise and TKE, but will persist more downstream NASA Langley Research Center May 8, 2006

15 Chevrons Add Vorticity
Pylon Plug Core Cowl Axi cross flow is symmetric, so axial vorticity = zero bb shows boundary layer vorticity shifted off axis by pylon RT longer chevrons show increased vorticity over RR and shorter chevrons on bottom show decreases NASA Langley Research Center May 8, 2006

16 Pylon, Plug, Chevron Interaction
RT fan vortices more defined on top, less on bottom due to chevron length Vertical velocity component shows effect of pylon on cross flow: Axi shows Coanda effect on plug Pylon cases have expanded downward flow region to get around pylon to fill in plug Less downward movement in fan flow for RT NASA Langley Research Center May 8, 2006

17 Consolidation and Entrainment
Core and fan shear layer vorticity consolidates to form vortex pair RR vortex pair slightly stronger than bb RT vortex pair significantly weaker than bb and RR NASA Langley Research Center May 8, 2006

18 T-Fan Reduces Overall Mixing
RT local mixing proportional to chevron length RT decreases net mixing, extends core by ~ 1/2 D RR negligible mixing over bb NASA Langley Research Center May 8, 2006

19 Overall Jet Trajectory
Total Temperature Centroid bb and RR equivalent – symmetric chevron does not interact with pylon effect RT showing less downward movement – favorable interaction of asymmetric chevron with pylon effect NASA Langley Research Center May 8, 2006

20 Summary Overall mixing does not vary much between bb, RR and RT and is not indicative of noise in this study The T-Fan effect: Varies the strength azimuthally of the localized chevron vorticity Reduces the downstream large scale vorticies introduced by the pylon Delays the merger of the fan and core shear layers Reduces peak noise and shifts it downstream There is the possibility of a more favorable design for shear layer merger, which can now be found computationally NASA Langley Research Center May 8, 2006

21 Concluding Remarks A predictive capability linking geometry to noise has been demonstrated The T-Fan benefits from a favorable interaction between asymmetric chevrons and the pylon effect NASA Langley Research Center May 8, 2006

22 Discussion, Extra Slides…
NASA Langley Research Center May 8, 2006

23 Axisymmetric Nozzle Surfaces colored by temperature
NASA Langley Research Center May 8, 2006

24 Baseline Nozzle (bb) Near surface streamlines and temperature
Fan boundary streamline NASA Langley Research Center May 8, 2006

25 Reference Chevrons (RR)
Near surface streamlines and temperature Slight upward movement NASA Langley Research Center May 8, 2006

26 PAA T-Fan Nozzle (RT) Near surface streamlines and temperature
Further upward movement NASA Langley Research Center May 8, 2006

27 Motivation Propulsion Airframe Aeroacoustics (PAA)
Definition: Aeroacoustic effects associated with the integration of the propulsion and airframe systems. Includes: Integration effects on inlet and exhaust systems Flow interaction and acoustic propagation effects Configurations from conventional to revolutionary PAA goal is to reduce interaction effects directly or use integration to reduce net radiated noise. NASA Langley Research Center May 8, 2006

28 PAA on QTD2: Concept to Flight in Two Years
Exploration of Possible PAA Concepts with QTD2 Partners (5/03 – 4/04) Extensive PAA CFD/Prediction Work (10/03 – 8/05) (AIAA , ) PAA Experiment at Boeing LSAF 9/04 PAA Effects and Noise Reduction Technologies Studied AIAA , , PAA on QTD2 – 8/05 PAA T-Fan Chevron Nozzle PAA Effects Instrumentation AIAA , NASA Langley Research Center May 8, 2006

29 Grid Coarse in Radial Direction
NASA Langley Research Center May 8, 2006

30 Grid Cause of Vorticity Lines
NASA Langley Research Center May 8, 2006

31 PAA Analysis Process to Develop Understanding of PAA T-fan Nozzle’s Flow/Noise Source Mechanisms
Begin with Highly Complex LSAF Jet-Pylon Nozzle Geometries JET3D Validation of Spectra Trend at 90 degrees Detailed PAA Flow Analysis Three major effects to understand: Pylon effect Chevron effect PAA T-fan effect and their interaction JET3D Noise Source Map Trends Validated with LSAF Phased Array Measurements Develop Linkages of complex flow and noise source interactions NASA Langley Research Center May 8, 2006


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