2 research outputs found
μΆμ μ΄μμ μ νΈλ‘λΆν° λ°μνλ 곡λ ₯-μν₯ μλ ₯ νμ€μ μν ꡬ쑰 μλ΅ μ°κ΅¬
νμλ
Όλ¬Έ (λ°μ¬) -- μμΈλνκ΅ λνμ : 곡과λν ν곡μ°μ£Όκ³΅νκ³Ό, 2021. 2. μ μμ€.The noise generated by the supersonic jet is a principal source of structural vibration and internal noise during the launching event or static-firing operations. Complex phenomena are observed due to the interaction between the aerodynamic, acoustic and vibratory loads. In this dissertation, linearized aero-acoustics and structural analyses are performed via the numerical simulation and further validated with experimental results obtained by the small-scale article test for a supersonic free-jet. For the numerical simulation, three-dimensional computational fluid dynamics(CFD), especially Reynolds averaged Navier-Stokes simulation(RANS) and delayed detached eddy simulation(DDES), are conducted. It is in order to explain the generation and propagation mechanism of the acoustic wave and reasonably calculate acoustic variables such as static pressure and its spatial/transient derivatives. Kirchhoff surface is placed at a distance to avoid the nonlinear turbulent sound-producing region. Helmholtz-Kirchhoff(H-K) method is employed in order to predict far field acoustic noise by using stored calculation results obtained by CFD at Kirchhoff surface. The Acceleration power spectral density(APSD) is predicted by employing a finite element method. The Optimal membrane element and discrete Kirchhoff triangle plate bending element(OPT-DKT) and Newmark-Ξ² time integration scheme are utilized in order to reduce discrepancies in lower to mid frequency response of the structure. Using the present CFD and H-K method, sound pressure level(SPL)s are quantitatively compared with experimental results measured by 12 and 15 microphones at near and far field, respectively. Moreover, APSD's are compared with the experimental results obtained by an accelerometer at three different locations. The objective of this dissertation is to establish an estimation procedure for vibratory responses of structure due to the aero-acoustic pressure generated from the supersonic jet noise in lower to mid frequencies.μν₯ νμ€μ μν ꡬ쑰 μ§λμ μ΄κ³ μλΉν체 λλ μ°μ£Όλ°μ¬μ²΄κ° λ°μ¬λ λ λ°μνλ λνμ μΈ νμμ΄λ€. μν₯ νμ€μ μν ꡬ쑰 μ§λ νμμ μμΈ‘νκΈ° μν΄μλ μ λ νμ€, μν₯ νμ€ λ° κ΅¬μ‘° μλ΅ λ± λ€λ¬Όλ¦¬ ν΄μμ΄ μꡬλλ€. λ³Έ λ
Όλ¬Έμμλ 곡λ ₯-μν₯-ꡬ쑰 μ§λ ν΄μμ μννμ¬ μΆμ μ΄μμ μ νΈλ‘λΆν° λ°μνλ 곡λ ₯-μν₯ μλ ₯μ μν ꡬ쑰 μλ΅ μ°κ΅¬λ₯Ό μννμμΌλ©° μ§μ μ€νμ μννμ¬ κ²°κ³Όλ₯Ό λΉκ΅νμλ€. 첫째, RANS λ° DDES μ μ°μ 체ν΄μμ μννμ¬ μΆμ μ΄μμ μ νΈμ μμ μμ± μ리 λ° μν₯ λ³μλ₯Ό μμΈ‘νμλ€. μν₯ λ³μλ₯Ό μ΄μ©νμ¬ κ·Όκ±°λ¦¬μ₯ μμμ ν¬κΈ°λ₯Ό μμΈ‘νμκ³ Kirchhoff νλ©΄μ μ΄μ©ν Helmholtz-Kirchhoff κΈ°λ²μ μ΄μ©νμ¬ μ거리μ₯ μμ ν¬κΈ°λ₯Ό μμΈ‘νμλ€. λμ§Έ, μ νμμ ν΄μμ μ΄μ©νμ¬ κ΅¬μ‘°λ¬Όμ μλ΅ μ°κ΅¬λ₯Ό μννμλ€. OPT-DKT μ μμ λ° Newmark-Ξ² κΈ°λ²μ μ΄μ©νμ¬ κ΅¬μ‘°λ¬Όμ κ°μλ μ€ννΈλΌμ μμΈ‘νμλ€. λν μΆμ μ΄μμ μ νΈμ λν μ€νμ μννμλ€. λ§μ΄ν¬λ‘ν° λ° κ°μλκ³λ₯Ό μ΄μ©νμ¬ κ·Όκ±°λ¦¬/μ거리μ₯μμμ μμμ ν¬κΈ° λ° κ΅¬μ‘°λ¬Όμ κ°μλ μ€ννΈλΌμ μΈ‘μ νμλ€. μμΈ‘λ 근거리μ₯μμμ μμμ ν¬κΈ°λ μ€ν κ²°κ³Όμ νκ· 4dB, μ거리μ₯μμμ μμμ ν¬κΈ°λ νκ· 2dB μ΄λ΄μ μ νμ±μ νμΈνμλ€. λν 곡λ ₯-μν₯ μλ ₯ νμ€μ μν΄ μ§λνλ ꡬ쑰물μ 3,000[Hz]κΉμ§ κ°μλ μ€ννΈλΌ μ λ’° μ£Όνμ λ²μκ° μμμ νμΈνμλ€. λ³Έ λ
Όλ¬Έμ λͺ©μ μ μΆμ μ΄μμ μ νΈμμ μμ±λλ 곡λ ₯-μν₯ μλ ₯ νμ€μ μν΄ μ§λνλ ꡬ쑰물μ μ μ£Όν~μ€μ£Όν μλ΅μ μμΈ‘νλ κ²μ΄λ€.Abstract i
Contents iii
List of Tables vi
List of Figures viii
Chapter 1 Introduction 1
1.1 Background 1
1.1.1 Aero-acoustic loads 1
1.1.2 Vibro-acoustic loads 4
1.2 Literature survey 5
1.2.1 Review of the aero-acoustic prediction for supersonic jet 5
1.2.2 Review of the vibro-acoustic prediction for launch vehicle structures 13
1.3 Aims and Scope 15
1.4 Outline of Dissertation 18
Chapter 2 Aero-acoustic prediction for supersonic jet 20
2.1 Governing equation for three-dimensional fluid dynamics 20
2.1.1 Reynolds averaged Navier Stokes equation 20
2.1.2 Large eddy simulation 23
2.1.3 Delayed detached eddy simulation 25
2.2 Boundary element method for CFD near field to the acoustic far field 27
2.2.1 Helmholtz-Kirchhoff method 27
Chapter 3 Experimental setup for a small-scale supersonic jet 29
3.1 Configuration of the small-scale supersonic jet 29
3.2 Experimental configuration for a small-scale supersonic jet 32
3.2.1 Near-field microphone array 34
3.2.2 Fear-field microphone array 37
Chapter 4 Aero-acoustic prediction and validation for the supersonic jet noise 40
4.1 Computational approach for the supersonic jet noise prediction 42
4.2 Validation of RANS and DDES 50
4.3 Near-field noise prediction and validation 54
4.4 Far-field noise prediction and validation 58
4.5 Discussion for the supersonic jet noise prediction and validation 63
4.5.1 Comparison of the numerical and experimental results 64
4.5.2 Effects of Kirchhoff surface location 68
4.5.3 Possibility of the crackle phenomena for the small-scale supersonic jet 71
Chapter 5 Vibro-acoustic analysis for a clamped thin plate structure 73
5.1 OPT-DKT shell element 75
5.2 Modal analysis of a clamped thin plate 80
5.3 Frequency response function of a clamped thin plate 83
5.4 Mesh convergence examination for the frequency response function 87
Chapter 6 Structural responses due to the aero-acoustic pressure 93
6.1 Computational approach for the vibro-acoustic analysis 94
6.2 Experiments for a clamped thin plate with an accelerometer 96
6.3 Equivalent modeling for the computational analysis 98
6.4 Validation of the present vibro-acoustic analysis 100
6.5 Discussion for structural responses predicting capability due to the aero-acoustic pressure 103
6.5.1 Natural frequencies of a clamped thin plate obtained by the experimental results 104
6.5.2 Maximum reliable frequency and the shifting effects 105
Chapter 7 Conclusion 109
7.1 Summary 109
7.2 Contributions of the present thesis 111
7.3 Future suggestions 113
Reference 114Docto