- Page 1: Technische Universität München In
- Page 5: Abstract - Zusammenfassung Due to t
- Page 8 and 9: CONTENTS 3.3.1.3 Boundary condition
- Page 10 and 11: Nomenclature Latin letters A area [
- Page 12 and 13: Nomenclature s t turbulent flame sp
- Page 14 and 15: Nomenclature Indices 0 ambient stat
- Page 16 and 17: Introduction band
- Page 18 and 19: Introduction Plenum Fuel Supply Com
- Page 20 and 21: Introduction 2) equivalence ratio f
- Page 22 and 23: Introduction drives oscillations [1
- Page 24 and 25: Introduction of th
- Page 26 and 27: Introduction The work starts with a
- Page 28 and 29: Introduction perfect premixed combu
- Page 30 and 31: Introduction 16
- Page 32 and 33: Numerical analysis of</stro
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Numerical analysis of</stro
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Numerical analysis of</stro
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Numerical analysis of</stro
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Acoustics The term D Dt = ∂ + u·
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Acoustics If the flow is homentropi
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Acoustics (3.6)) yields: p ′ = c
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Acoustics In case of</stron
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Acoustics Fuel Supply Air Supply Pl
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Acoustics Beside the transfer matri
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Acoustics much smaller than the sho
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Acoustics i L j i j f j g j k f i f
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Acoustics c 2 j c 2 i = 1+ γ−1
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Acoustics can be rewritten in terms
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Acoustics velocity fluctuations. Th
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Acoustics 2 1.5 |det(S)| 1 0.5 0 46
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Acoustics 68
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Modeling of turbul
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Modeling of turbul
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Modeling of turbul
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Modeling of turbul
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Modeling of turbul
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Modeling of turbul
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System Identification idation <stro
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System Identification x (1) x (2) x
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System Identification The second te
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System Identification T c = m∆t ,
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System Identification to satisfy ce
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System Identification 5.5 Pro<stron
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System Identification Phase Amplitu
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System Identification Amplitude 0.2
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System Identification 0.2 0.15 0.1
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System Identification the other two
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System Identification 0.15 0.1 Ampl
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System Identification 1 0.9 Quality
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Numerical simulation 0.00816 m 2 .
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Numerical simulation tors i = 2 for
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Numerical simulation can be calcula
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Numerical simulation Velocity inlet
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Numerical simulation aCFL=(u+ c)
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Numerical simulation 2000 1500 Coun
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Numerical simulation 0.02 Amplitude
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Numerical simulation 6.3.1 Combusto
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Numerical simulation Phase Amplitud
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Numerical simulation 0.06 0.04 0.02
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Numerical simulation Phase Amplitud
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Numerical simulation 6.3.3 Analysis
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Numerical simulation 0.1 0.05 Ampli
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Numerical simulation towards the bu
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Numerical simulation area, which is
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Numerical simulation 3.14 3.14 Phas
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Numerical simulation The length <st
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Acoustic analysis model of<
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Acoustic analysis Figure 7.2: Finit
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Acoustic analysis = F u (ω) u′ b
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Acoustic analysis ply could change
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Acoustic analysis 1.5 100 10 (CI
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Acoustic analysis 3.14 1.57 Phase 0
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Acoustic analysis Amplitude 0.01 0.
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Acoustic analysis 3.14 1.57 Phase 0
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Acoustic analysis Phase Amplitude 5
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Acoustic analysis 0.2 0.1 (CI − 1
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Acoustic analysis 1 100 10 (CI −
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Acoustic analysis Amplitude 0.3 0.2
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Acoustic analysis 1 10 1 (CI − 1)
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Acoustic analysis how effective it
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Summary and Conclu
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Summary and Conclu
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BIBLIOGRAPHY 2001: Power for L<stro
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BIBLIOGRAPHY [28] S. Evesque <stron
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BIBLIOGRAPHY [45] J.D. Holdemann, D
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BIBLIOGRAPHY [62] Klaas Kunze. Unte
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BIBLIOGRAPHY [82] M.L. Munjal. Acou
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BIBLIOGRAPHY [102] W. Polifke, A. P
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BIBLIOGRAPHY [121] T. Schuller, D.
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A Appendix A.1 Transformation <stro
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188 Figure A.1: Sketch of</
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Appendix T-junctions A i [m 2 ] A j