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Multi-source Aeroacoustic Noise Prediction Method Jonathan SCOTT CFD Engineer 03/12/2013 1 Issue 01 APR2012, RCO-F-DSE-4051 Introduction Trend to reduce engine displacement while increasing break power by turbo charging engines


  1. Multi-source Aeroacoustic Noise Prediction Method Jonathan SCOTT CFD Engineer 03/12/2013 1 Issue 01 APR2012, RCO-F-DSE-4051

  2. Introduction  Trend to reduce engine displacement while increasing break power by turbo charging engines  Traditionally GT Power and Wave are used for predicting engine order content when developing exhaust systems  Our company has had mixed results using a combination of RANS/Vnoise  Rule of thumb; maximum mach number < 0.25 Property of Faurecia - Duplication prohibited  The latter inherently assumes aero-acoustic sources are solely dependent on Mach number Issue 01 APR2012, RCO-F-DSE-4051

  3. Test data of Sound power against Mach number for pipes with an outer diameter of 1.75” All bends Straight pipe ~ 6 dB Sound Power (dB) Property of Faurecia - Duplication prohibited Mach number Looking at Mach Numbers in the tailpipe does not alleviate all concern for flow noise Issue 01 APR2012, RCO-F-DSE-4051

  4. Review of available aero-acoustics methods  DNS Not feasible for our Predict all eddie scales directly to solve the Navier- applications and Stokes equations resources  RANS Does n’t capture the The averaged version of the Navier-Stokes equation physics completely, are solved along with another equation to represent aero-acoustic all turbulent scales. analogies have Only the effect of eddies on the mean flow are shown some success captured Property of Faurecia - Duplication prohibited  Vnoise Still limited by the RANS input, The use of a RANS simulation as an input into a additional software, noise propagation software and captures the time and resources propagation to the desired microphones. required, mixed success Issue 01 APR2012, RCO-F-DSE-4051

  5. Multi-source Aeroacoustic Noise  RANS with an acoustic analogy seems to offer the best solution  Initial objective was to develop a methodology which is within 3 dB of measurements and create a tailpipe design guideline  Chosen to use the Proudman acoustic analogy Property of Faurecia - Duplication prohibited Issue 01 APR2012, RCO-F-DSE-4051

  6. Background Fluid Dynamics Pipe bend Jet noise  The first is caused by flow separation around pipe bends Property of Faurecia - Duplication prohibited  The second is commonly known as “jet noise” Issue 01 APR2012, RCO-F-DSE-4051

  7. Proudman analogy (Lilley)  The acoustic power, AP per unit volume (W/m 3 ) STAR-CCM+ manual  The total acoustic power per unit volume can be reported in dB: STAR-CCM+ manual  Where (P ref ) is the reference acoustic power; 10e-12 W/m 3  Using the classical summation for multiple acoustic sources [2], the total sound power can be found   SPL n  i Property of Faurecia - Duplication prohibited   [2]  10 SPL 10 log 10   T 10    i 1  The largest total is when both sources are the same value and thus the total is 3 dB louder than the single source. Issue 01 APR2012, RCO-F-DSE-4051

  8. Adjusted Proudman sources Wake Bend region region Proudman adjusted wake + C 1 [3] Property of Faurecia - Duplication prohibited Proudman adjusted bend + C 2 [4] Issue 01 APR2012, RCO-F-DSE-4051

  9. RANS CFD Methodology  2mm cell size in the wake  Volume refinement around the pipe bend  A low Reynolds mesh Property of Faurecia - Duplication prohibited  The K-omega SST model Issue 01 APR2012, RCO-F-DSE-4051

  10. Typical flow for a 90 ° bend 0 deg 45 deg Axial Radial Axial Radial 90 deg 1D downstream Axial Radial Axial Radial Property of Faurecia - Duplication prohibited Radial flow magnitude can be 2/3 of the axial mean flow so the secondary flow can be quite strong. Issue 01 APR2012, RCO-F-DSE-4051

  11. Typical flow for a 90 ° bend Velocity Turbulent Kinetic Energy Proudman Acoustic Power Proudman Acoustic Power Property of Faurecia - Duplication prohibited Issue 01 APR2012, RCO-F-DSE-4051

  12. Parts tested Do: Outer pipe diameter r r: Inner pipe radius Rc: Radius of curvature of bend Rc Rc/r: Bend ratio Straight pipes Bent pipes Do: 57 mm, Rc/r: 3.2 Do: 45 mm, Rc/r: 4.2 Do: 45 mm, Rc/r: 3.6 Property of Faurecia - Duplication prohibited Do: 45 mm, Rc/r: 3.0 Do: 55 mm Do: 50 mm Do: 45 mm Issue 01 APR2012, RCO-F-DSE-4051

  13. Comparison of test data to Proudman analogy Straight pipe Do: 45mm Test Proudman Proudman corrected Sound Power (dB) Property of Faurecia - Duplication prohibited Flow rate (SCFM) With the Proudman correction [3], the correlation is excellent Issue 01 APR2012, RCO-F-DSE-4051

  14. Comparison of test data to Proudman analogy For all straight pipes Test Proudman corrected Sound Power (dB) Property of Faurecia - Duplication prohibited Mach number Proportional relationship between sound power and Mach Number for straight pipes Issue 01 APR2012, RCO-F-DSE-4051

  15. Comparison of test data to Proudman analogy For the bent pipes Test Wake Total Sound Power (dB) Average Δ ~ 2 dB Property of Faurecia - Duplication prohibited 1 2 3 4 5 6 7 8 Case number Using Proudman with correction [3] and integrating over the whole region (Total), the sound power is always underpredicted Issue 01 APR2012, RCO-F-DSE-4051

  16. Comparison of test data to Proudman analogy For the bent pipes Test Wake Total with bend adjust Sound Power (dB) Average Δ < 1 dB Property of Faurecia - Duplication prohibited 1 2 3 4 5 6 7 8 Case number Integrating separately for each source region and applying an adjustment to the bend source strength [4] the average difference was reduced to less than 1 dB Issue 01 APR2012, RCO-F-DSE-4051

  17. CFD predictions for a range of sizes available from our prototype shop Sound Power (dB) Do: 45 mm, Angle: 60 deg Do: 45 mm, Angle: 90 deg Property of Faurecia - Duplication prohibited Do: 57 mm, Angle: 60 deg Do: 57 mm, Angle: 60 deg Bend ratio Populate the range of sizes from our prototype shop, now we can create a design guideline to reduce flow noise based upon bend ratio Issue 01 APR2012, RCO-F-DSE-4051

  18. Conclusions  Aero-acoustics prediction within 1 dB using the Proudman analogy and two small correction factors  Quantifying the contribution of each source is easy to implement via field functions  Design guideline was populated so that we can minimize aero-acoustic noise Property of Faurecia - Duplication prohibited Issue 01 APR2012, RCO-F-DSE-4051

  19. Future  Additional sizes from our prototype shop need to be added to the design chart  Further testing required to understand how the distance between the pipe bend and tailpipe exit affect the sound power  INCE paper, submission pending Property of Faurecia - Duplication prohibited Issue 01 APR2012, RCO-F-DSE-4051

  20. Questions ? ? ? Property of Faurecia - Duplication prohibited Issue 01 APR2012, RCO-F-DSE-4051

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