Aeroacoustics of Three-Stream Jets Brenda Henderson* NASA Glenn - - PowerPoint PPT Presentation

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Aeroacoustics of Three-Stream Jets Brenda Henderson* NASA Glenn - - PowerPoint PPT Presentation

https://ntrs.nasa.gov/search.jsp?R=20120018041 2018-06-05T20:34:36+00:00Z Aeroacoustics of Three-Stream Jets Brenda Henderson* NASA Glenn Research Center, Cleveland, OH Results from acoustic measurements of noise radiated from a heated,


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SLIDE 1

Aeroacoustics of Three-Stream Jets

Brenda Henderson* NASA Glenn Research Center, Cleveland, OH Results from acoustic measurements of noise radiated from a heated, three-stream, co-annular exhaust system operated at subsonic conditions are presented. The experiments were conducted for a range of core, bypass, and tertiary stream temperatures and pressures. The nozzle system had a fan-to-core area ratio of 2.92 and a tertiary-to-core area ratio of 0.96. The impact of introducing a third stream on the radiated noise for third-stream velocities below that of the bypass stream was to reduce high frequency noise levels at broadside and peak jet- noise angles. Mid-frequency noise radiation at aft observation angles was impacted by the conditions of the third stream. The core velocity had the greatest impact on peak noise levels and the bypass-to-core mass flow ratio had a slight impact on levels in the peak jet-noise

  • direction. The third-stream jet conditions had no impact on peak noise levels. Introduction of a

third jet stream in the presence of a simulated forward-flight stream limits the impact of the third stream on radiated noise. For equivalent ideal thrust conditions, two-stream and three- stream jets can produce similar acoustic spectra although high-frequency noise levels tend to be lower for the three-stream jet.

https://ntrs.nasa.gov/search.jsp?R=20120018041 2018-06-05T20:34:36+00:00Z

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SLIDE 2

Fundamental Aeronautics Program

Supersonics Project

National Aeronautics and Space Administration

Aeroacoustics of Three-Stream Jets

Brenda Henderson, NASA Glenn Research Center

18th AIAA/CEAS Aeroacoustics Conference June 4 – 6, 2012 Colorado Springs, Colorado

www.nasa.gov

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SLIDE 3

Purpose of Study

  • Understand noise reduction potential of a third stream that

may be available in future engine architectures

  • Most straight-forward use of third stream is as an additional

bypass stream

  • Need to predict noise from three-stream jets – current semi-

empirical tools address single and dual stream jets

  • Results of co-annular studies may guide other three-stream

concepts (ejector)

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SLIDE 4

Aero-Acoustic Propulsion Laboratory (AAPL)

NATR Microphone Array HFJER

  • AAPL

‒ 66 foot geodesic dome ‒ 45 foot microphone arc – 24 elements

  • Nozzle Acoustic Test Rig (NATR)

‒ 53 inch simulated flight stream ‒ Maximum Mach number = 0.35

  • High Flow Jet Exit Rig (HFJER)

‒ 3-stream capability (3rd stream new) ‒ Independent pressure control on all streams ‒ Independent temperature control on fan and core streams ‒ Fan and third-stream temperatures the same

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SLIDE 5

Model Hardware

Core Nozzle Fan Stream Third-Stream Nozzle

  • Core stream nozzles
  • Round
  • Lobed mixer
  • 4.8 inch exit diameter
  • Fan-to-core area ratio = 2.92 (fixed)
  • Tertiary-to-core area ratio = 0.92 (fixed)

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SLIDE 6

Cycle Points

NPRc NPRb NPRt NTRc Mfj = 0 Mfj = 0.2 Mfj = 0.3 1.5 1.5 1.0 - 1.5 2.8

1.6 1.6 1.0 - 1.6 2.8

1.7 1.7 1.0 - 1.7 2.8

1.8 1.8 1.0 - 1.8 2.8

1.5 1.5 1.0 - 1.5 3.2

1.5 1.4 1.0 - 1.4 3.2

1.5 1.6 1.0 - 1.6 3.2

1.6 1.5 1.0 - 1.5 3.2

 

1.6 1.6 1.0 - 1.6 3.2

 

1.6 1.7 1.0 - 1.7 3.2

 

1.7 1.6 1.0 - 1.6 3.2

  

1.7 1.7 1.0 - 1.7 3.2

  

1.7 1.8 1.0 - 1.8 3.2

  

1.8 1.7 1.0 - 1.7 3.2

 

1.8 1.8 1.0 - 1.8 3.2

  

  • Mfj – free jet (simulated flight stream) Mach number
  • NPR – nozzle pressure ratio
  • NTR – nozzle temperature ratio

Subsonic Exhausts

Baseline Experiments

NTRb = 1.25

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SLIDE 7

Data Analysis

  • Baseline Experiments

– NPRc = NPRf = 1.8, 1 < NPRt < 1.8 – NTRc = 3.2 – Mfj = 0

  • Reduced velocity of all streams
  • Changed velocity ratio (Vb/Vc)
  • Impact of velocity and bypass ratio
  • Impact of simulated flight stream
  • Impact of partially mixed flow
  • Comparison on equal thrust basis
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SLIDE 8

Repeat Acquisitions

NPRc NPRb NPRt 90o 150o

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SLIDE 9

Smoothed Data

90o 150o

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Baseline Results

90o 150o NTRc = 3.2

Simulated 2-Stream Jet, BPRfan/core = 4.7 Simulated 2-Stream Jet, BPRfan/core = 6.3 Trailing Edge Tones

Vb/Vc = 0.62 Wb/Wc = 4.7

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SLIDE 11

Reduced Pressure/Velocity

90o NTRc = 3.2 150o

Vb/Vc = 0.62 Wb/Wc = 4.6

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SLIDE 12

Increased Velocity Ratio (Vb/Vc)

90o NTRc = 2.8 150o

Vb/Vc = 0.66 Wb/Wc = 4.3

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SLIDE 13

Reduced Velocity Ratio (Vb/Vc)

90o NTRc = 3.2 150o

Vb/Vc = 0.59 Wb/Wc = 3.7

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SLIDE 14

Impact of Velocity and Bypass Ratio

NTRc = 3.2

Vb/Vc = 0.66, Wb/Wc = 4.3 Vb/Vc = 0.65, Wb/Wc = 6.0

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90o 150o

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SLIDE 15

Impact of Simulated Forward Flight

150o 90o

NTRc = 3.2 Mfj = 0.3

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SLIDE 16

Impact of Partially Mixed Core and Fan

150o 90o

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NTRc = 3.2 Mfj = 0.3

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SLIDE 17

Equal Thrust Comparisons

150o 90o

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SLIDE 18

Conclusions

  • Addition of a third stream reduced high-frequency noise and

impacted mid-frequency noise

  • The presence of a simulated flight stream reduced the

impact of the third stream

  • The core-stream velocity had the greatest impact of all

parameters investigated on the radiated noise

  • Comparisons on an equal thrust basis show that three-

stream jets are not inherently quieter than two-stream jets