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Identification of Swirl Waves using Local Stability Analysis

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1 Identification of Swirl Waves using Local Stability Analysis
Alp Albayrak, Wolfgang Polifke

2 2 distinct propagation scales are present
Acoustic wave propagation ๐‘ข ๐‘ = ๐‘ข ๐‘ฅ ยฑ๐‘ Swirl wave propagation ๐‘ข ๐‘ = ๐‘ข ๐‘ฅ ๐‘ข ฮธ โ€ฒ ๐‘ข ๐‘ง โ€ฒ ๐‘ข ๐‘ง ๐‘ข ฮธ Swirler

3 Recap from ICSV22: Swirl waves are not convective
๐‘ข ฮธ โ€ฒ ๐‘ข ฮธ ๐‘ข ฮธ ๐‘ฅ Output Plane Constant Speed Model Input Plane Current Model CFD Result

4 Modal decomposition can easily describe the propagation speeds.
Linearized NS Eq: ๐‘ข โ€ฒ ๐‘ก,๐‘ง,๐‘Ÿ =๐‘ข ๐‘ก,๐‘ง,๐‘Ÿ โˆ’ ๐‘ข ๐‘ง,๐‘Ÿ ๐œ• ๐‘ข ๐‘Ÿ โ€ฒ ๐œ•๐‘ก + ๐‘ข ๐‘ง ๐œ• ๐‘ข ๐‘Ÿ โ€ฒ ๐œ•๐‘ง โˆ’ 2 ๐‘ข ๐œƒ ๐‘ข ๐œƒ โ€ฒ ๐‘Ÿ =โˆ’ 1 ๐œŒ ๐œ• ๐‘ โ€ฒ ๐œ•๐‘Ÿ +๐œ 1 ๐‘Ÿ ๐œ• ๐‘ข ๐‘Ÿ โ€ฒ ๐œ•๐‘Ÿ + ๐œ• 2 ๐‘ข ๐‘Ÿ โ€ฒ ๐œ• ๐‘Ÿ ๐œ• 2 ๐‘ข ๐‘Ÿ โ€ฒ ๐œ• ๐‘ง 2 โˆ’ ๐‘ข ๐‘Ÿ โ€ฒ ๐‘Ÿ 2 Normal Modes: ๐‘ข ๐‘Ÿ = ๐‘ข โ€ฒ ๐‘ก,๐‘ง,๐‘Ÿ ๐‘’๐‘ฅ๐‘ ๐‘– โˆ’๐œ”๐‘ก+๐‘˜๐‘ง โˆ’๐‘–๐œ” ๐’– ๐’“ +๐‘–๐‘˜ ๐‘ข ๐‘ง ๐’– ๐’“ โˆ’ 2 ๐‘ข ๐œƒ ๐‘Ÿ ๐’– ๐œฝ =โˆ’ 1 ๐œŒ ๐‘‘ ๐’‘ ๐‘‘๐‘Ÿ +๐œ 1 ๐‘Ÿ ๐‘‘ ๐’– ๐’“ ๐‘‘๐‘Ÿ + ๐‘‘ 2 ๐’– ๐’“ ๐‘‘ ๐‘Ÿ 2 โˆ’ ๐‘˜ 2 ๐’– ๐’“ โˆ’ ๐’– ๐’“ ๐‘Ÿ 2 Temporal analysis: fix ๐‘˜โˆˆโ„, find ฯ‰ ๐‘› โˆˆโ„‚ and ๐‘‹ ๐‘› ๐‘Ÿ โˆˆโ„‚ ๐‘ข ๐‘ ๐‘› = ๐‘…๐‘’ ๐œ” ๐‘› ๐‘˜

5 Eigenvalue problem is constructed from modal decomposition and is easy to solve.
๐œ๐‘˜ 2 + ๐œ ๐‘Ÿ 2 +๐‘–๐‘˜ ๐‘ข ๐‘ง โˆ’ ๐œ๐ท ๐‘Ÿ โˆ’๐œ ๐ท 2 ๐‘ข ๐‘Ÿ โˆ’ 2 ๐‘ข ๐œƒ ๐‘Ÿ ๐‘ข ๐œƒ + ๐ท ๐œŒ ๐‘ =๐‘–๐œ” ๐‘ข ๐‘Ÿ ๐ด ๐‘˜ ๐‘ข =๐œ”๐ต ๐‘ข ๐ด 11 ๐ด ๐ด โ‹ฏ ๐ด 1๐‘› ๐ด ๐ด โ‹ฎ โ‹ฑ โ‹ฎ ๐ด ๐ด ๐ด ๐‘š1 โ‹ฏ ๐ด ๐ด ๐ด ๐‘š๐‘› ๐‘ข ๐‘ง โ‹ฎ ๐‘ข ๐‘Ÿ โ‹ฎ ๐‘ข ๐œƒ โ‹ฎ ๐‘ โ‹ฎ =๐œ” ๐ต 11 ๐ด ๐ด โ‹ฏ ๐ต 1๐‘› ๐ด ๐ด โ‹ฎ โ‹ฑ โ‹ฎ ๐ด ๐ด ๐ต ๐‘š1 โ‹ฏ ๐ด ๐ด ๐ต ๐‘š๐‘› ๐‘ข ๐‘ง โ‹ฎ ๐‘ข ๐‘Ÿ โ‹ฎ ๐‘ข ๐œƒ โ‹ฎ ๐‘ โ‹ฎ

6 Each mode has its own growth rate ๐œ” ๐‘– and propagation speed ๐œ” ๐‘Ÿ ๐‘˜ Propagation speeds are clustered around convective speed. Convection speed Analytical Model: (๐‘ข ๐‘ ) ๐‘š๐‘Ž๐‘ฅ =1.46 (๐‘ข ๐‘ ) ๐‘š๐‘–๐‘› =0.54 Growth Rate Propagation speed

7 Oscillatory modes are damped faster.
( ๐‘ข ๐œƒ )

8 Quantitative comparison is missing: Construct IR
Next steps Quantitative comparison is missing: Construct IR

9 Analytical approach reveals important criteria for swirl waves.
๐ถ ๐‘ข ๐œƒ +๐‘ฉ ๐‘ข ๐‘Ÿ =0 2 ๐‘ข ๐œƒ ๐ถ๐‘Ÿ ๐‘ข ๐œƒ โˆ’ ๐‘ข ๐‘Ÿ + 1 ๐‘˜ 2 ๐‘‘ 2 ๐‘ข ๐‘Ÿ ๐‘‘ ๐‘Ÿ ๐‘Ÿ ๐‘‘ ๐‘ข ๐‘Ÿ ๐‘‘๐‘Ÿ โˆ’ ๐‘ข ๐‘Ÿ ๐‘Ÿ 2 =0 ๐ถ=๐‘– ๐‘˜ ๐‘ข ๐‘ง โˆ’๐œ” is convective operator. ๐‘ฉ= ๐‘ข ๐œƒ ๐‘Ÿ + ๐‘‘ ๐‘ข ๐œƒ ๐‘‘๐‘Ÿ , ๐‘ข ๐œƒ =๐พ ๐‘Ÿ ๐‘› โ†’ ๐‘›<โˆ’1โ†’๐ต<0 ๐‘›=โˆ’1โ†’๐ต=0 ๐‘›>โˆ’1โ†’๐ต>0 (free vortex)

10 Non-convective waves are not present for free vortex
๐‘ข ๐œƒ =๐ถ ๐‘ข ๐œƒ =๐ถ๐‘Ÿ ๐‘ข ๐œƒ =๐ถ/ ๐‘Ÿ 2 ๐‘ข ๐œƒ =๐ถ/๐‘Ÿ ๐ต<0 ๐ต=0 ๐ต>0

11 Further research Construct IR for quantitative comparison.
Comparison with global stability analysis (more realistic profiles?) Build a model for ๐‘ข ๐œƒ โ€ฒ โ†’ ๐‘„ โ€ฒ

12 Identification of Swirl Waves using Local Stability Analysis
Alp Albayrak, Wolfgang Polifke

13 Oscillatory modes are damped faster.


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