4 research outputs found
Experimental Study on Flow Characteristics of Synthetic Jet with Circular Exit Array in Separated Flow
Piezo-electric diaphragmμΌλ‘ μλλλ synthetic jetμ λ°λ¦¬ μ λ μ μ΄μ μ μ©νκΈ° μν μ€νμ μννμ¬ μ μ° μμΉ ν΄μ κ²°κ³Όμ μ λ νμμ λΉκ΅ λΆμνμλ€. μΈλΆ μ λμ΄ μλ 쑰건μμ μ΄μ μ μκ³λ₯Ό νμ©ν μΆκ΅¬ μλ μΈ‘μ μ€νμ ν΅ν΄ μλ μ£Όνμμ μΆκ΅¬ μ§λ¦μ΄ μΆκ΅¬ μ μ λ³νμ μ€μν μν μ νκ³ μμμ κ²μ¦νλ€. μΆκ΅¬ λ¨λ©΄μ μ΄ λμΌν 쑰건μ μ€νμμλ λμΌν μ λμ΄ μΆκ΅¬λ₯Ό ν΅ν΄ λΆμΆλλλΌλ μΆκ΅¬ λλ μ κΈΈμ΄κ° 컀μ§μλ‘ μ μ±μ μν₯μ΄ μ¦κ°νμ¬ μΆκ΅¬ μ μμ΄ κ°μν¨μ μ μ μμλ€. μΈλΆ μ μ
λ₯κ° μλ inclined flat plateμμ synthetic jet μλ μ /νμ μλ ₯ κ³μ λΆν¬λ₯Ό λΉκ΅νμ¬ μ λ μ μ΄ μ±λ₯μ κ²°μ νλ ν΅μ¬ νλΌλ―Έν°μ μν μ κ²μ¦νλ€. κ·Έ κ²°κ³Ό μ£Όμ΄μ§ λ°λ¦¬ λ°μ 쑰건μμ μ΅μ μ μ λ μ μ΄ μ±λ₯μ λ°ννλ μλ μ£Όνμ, μΆκ΅¬ μ§λ¦, μΆκ΅¬ κ°κ²©μ λ°κ²¬ν μ μμλ€.The control of separated flow on an inclined flat plate using synthetic jet which actuated by piezo-electric diaphragm was investigated experimentally. Experimental results were compared with computational results in order to analyze flow physics. According to the result of jet velocity using hot wire anemometry with no cross flow, we found that actuation frequency and orifice diameter played important role in jet velocity. On the condition of same exit area, jet velocity was decreased because of exit perimeter which related with viscous effect. According to the result of measuring static pressure on the inclined flat plate with cross flow, we found that actuation frequency and orifice diameter and gap between orifices played important role in separation control performance.λ³Έ μ°κ΅¬λ λ°©μμ¬μ
μ² λ° κ΅λ°©κ³Όνμ°κ΅¬μ
(UC100031JD), μνΌμ»΄ν¨ν
μΌν°(KSC-2010-C1-
0030), ν곡 μ°μ£Ό μ κΈ°μ μ°κ΅¬μ, BK 21μ μ§μ
μΌλ‘ μνλμμ.OAIID:oai:osos.snu.ac.kr:snu2011-01/104/0000004648/24SEQ:24PERF_CD:SNU2011-01EVAL_ITEM_CD:104USER_ID:0000004648ADJUST_YN:NEMP_ID:A001138DEPT_CD:446CITE_RATE:0FILENAME:λ°°μ΄λ_μν_μΆκ΅¬_Synthetic_Jetμ_λ°λ¦¬_μ λ_μ μ΄_νΉμ±μ_κ΄ν_μ€νμ _μ°κ΅¬.pdfDEPT_NM:κΈ°κ³ν곡곡νλΆEMAIL:[email protected]:
Smart actuation for helicopter rotorblades
Successful rotorcrafts were only achieved when the differences between hovering flight conditions and a stable forward flight were understood. During hovering, the air speed on all helicopter blades is linearly distributed along each blade and is the same for each. However, during forward flight, the forward motion of the helicopter in the air creates an unbalance. The airspeed is increased for the blade passing in the advancing side of the helicopter, while it is reduced in the retreating side. Moreover, when each blade enters the retreating side of the helicopter, a reverse flow occurs around the profile where the blade speed is lower than the forward speed of the helicopter. The balance of a rotorcraft is solved by a cyclic pitch control, but trade-offs are made on the blade design to cope with the great variety of aerodynamic conditions. A smart blade that would adapt its characteristics to this large set of conditions would improve rotorcrafts energy efficiency while providing vibration and noise control.\ud
Smart rotor blades systems are studied to adapt the aerodynamic characteristics of the blade during its revolution and to improve the overall performances. An increase in the lift over drag ratio on the retreating side has been studied to design a blade with better aerodynamic efficiency and better stall performances in the low-speed region. The maximum speed of a rotorcraft is limited by the angle of attack that the profile can sustain on the retreating side before stall. Therefore, increasing the maximum angle of attack that a profile geometry can sustain increases the rotorcraft flight envelope. Flow asymmetry and aerodynamic interaction between successive blades are also investigated to actively reduce vibrations and limit noise.\ud
These improvements can be achieved by deploying flaps, by using flow control devices or by morphing the full shape of the profile at a specific places during the blade revolution. Each of the listed methods has advantages and disadvantages as well as various degrees of feasibility and integrability inside helicopter blades. They all modify the aerodynamic characteristics of the profile. Their leverage on the various aerodynamic effects depends on the control strategy chosen for actuation. Harmonic actuation is therefore studied for active noise and vibration control whereas stepped deployment is foreseen to modify the stall behaviour of the retreating side of the helicopter.\ud
Helicopter blades are subjected to various force constraints such as the loads from the complex airflow and the centrifugal forces. Furthermore, any active system embedded inside a rotor blade needs to comply with the environmental constraints to which a helicopter will be subjected Β during its life-span. Other concerns, like the power consumption and the data transfer for blade control, play an important role as well. Finally, such a system must have a life-time exceeding the life-time of a rotor blade and meet the same criteria in toughness, reliability and ease of maintenance.\ud
Smart system is an interplay of aerodynamics, rotor-mechanics, material science and control, thus a multidisciplinary approach is essential. A large part of the work consists in building processes to integrate these domains for investigating, designing and testing smart components.\ud
Piezoelectric actuators are a promising technology to bring adaptability to rotor blades. They can be used directly on the structure to actively modify its geometry, stiffness and aerodynamic behaviour or be integrated to mechanisms for the deployment of flaps. Their large specific work, toughness, reliability and small form factor make them suitable components for integration within a rotor blade. The main disadvantage of piezoelectric actuators is the small displacement and strain available. Amplification mechanisms must be optimised to produce sufficient displacement in morphing applications.\ud
Smart actuation systems placed inside rotor blades have the potential to improve the efficiency and the performances of tomorrow's helicopters. Piezoelectric materials can address many of the challenges of integrating smart components inside helicopter blades. The key aspect remains the collaboration between various domains, skills and expertise to successfully implement these new technologies
Synthetic jetμ μ΄μ©ν 3μ°¨μ λ κ° λ₯λ μ λμ μ΄μ κ΄ν μμΉμ μ°κ΅¬
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Όλ¬Έ (λ°μ¬)-- μμΈλνκ΅ λνμ : νλκ³Όμ κ³μ°κ³Όνμ 곡, 2014. 8. κΉμ’
μ.λ³Έ μ°κ΅¬λ 3μ°¨μ λ κ° νμμ 곡λ ₯ μ±λ₯μ ν₯μμν€κΈ° μνμ¬ synthetic jetμ μ΄μ©ν 곡λ ₯ νΉμ± ν₯μ λ©μ»€λμ¦μ κ΄νμ¬ μμΉμ μ°κ΅¬λ₯Ό μννμλ€. λ³Έ μ°κ΅¬λ₯Ό ν΅νμ¬ synthetic jetμ μΆκ΅¬ νμμ λ°λ₯Έ μ λ νΉμ± νμ
μ ν΅ν΄ μ λμ μ΄μ ν¨κ³Όμ μΈ μΆκ΅¬ νμμ λμΆνκ³ , μ΄λ‘λΆν° μ»μ synthetic jetμ νμμ 3μ°¨μ λ κ°μ μ μ©νμ¬ κ³ λ°μκ°μμμ λ°λ¦¬μ λ μ μ΄ νΉμ±μ λΆμνμλ€.
Synthetic jetμ μΆκ΅¬ νμμ jet vortexμ λ°λ¬ κ³Όμ λ° μ 체μ μΈ jet momentumμ μν₯μ μ£ΌκΈ° λλ¬Έμ μ λμ μ΄ νΉμ±μ ν° μν₯μ λ―ΈμΉλ μμΈ μ€ νλμ΄λ€. μ΄μ μ λμ μ΄μ ν¨κ³Όμ μΈ μΆκ΅¬ νμμ λμΆνκΈ° μν΄ ννμμ μ μ
λ₯κ° μ‘΄μ¬ν κ²½μ° μ¬κ°νκ³Ό μν μΆκ΅¬ νμμ λνμ¬ jet vortex μ λ ꡬ쑰 λ° μ λμ μ΄ κ°λ₯μ±μ λΆμνμλ€. μ¬κ°ν μΆκ΅¬ νμμ κ²½μ°, jet μΆκ΅¬ μ§νμμλ ν° μλ₯λ₯Ό λ°μμν€μ§λ§ μΆκ΅¬ λμμ λ°μνλ νμ μ λμ μν΄ jetμ μν ν¨κ³Όκ° κΈκ²©ν κ°μν¨μ νμΈνμλ€. μν μΆκ΅¬ νμμ κ²½μ°, μ¬κ°ν μΆκ΅¬ νμλ³΄λ€ κ· μΌν jet vortexλ₯Ό μμ±νκ³ μ μ
λ₯ λ°©ν₯μΌλ‘ λ³΄λ€ λ©λ¦¬κΉμ§ jetμ μν₯μ΄ λ―ΈμΉλ μ λꡬ쑰λ₯Ό κ°μ§κ³ μμ΄ μ¬κ°ν μΆκ΅¬ νμλ³΄λ€ μ λμ μ΄μ ν¨κ³Όμ μμ νμΈνμλ€. λν μν μΆκ΅¬ νμμ hole gapκ³Ό hole diameterμ λ³νμ λ°λ₯Έ μ λ ꡬ쑰 λ° μ λ νΉμ±μ λΉκ΅ λΆμν¨μΌλ‘μ¨ μ λμ μ΄ ν¨κ³Όλ₯Ό κ·Ήλν ν μ μλ μνμΆκ΅¬ νμμ λμΆνμλ€.
λ€μν μμΉ ν΄μ κ²°κ³Όμ λΆμμ ν΅ν΄μ λμΆλ μν μΆκ΅¬ νμμ synthetic jetμ μ μ©νμ¬ λ체-λ κ° νΌν© νμμ μ λμ μ΄λ₯Ό μννμλ€. νλ μ€νκ³Ό μμΉν΄μμ ν΅ν΄ λ°μκ°μ λ³νμ λ°λ₯Έ 3μ°¨μ λ κ°μ μ λ λΆμμ μνν κ²°κ³Ό, λ κ°μ λ°μκ° μ¦κ°μ λ°λΌ μμ μμλΆν° λ°μν μλ₯μ λμ λΆκ΄΄νκ² λλ©° λ κ° λ°κΉ₯μͺ½ λΆλΆμ μλΆν°λ λ°λ¦¬ μ λμ΄ λ°λ¬ν¨μ νμΈνμλ€. μ΄μ μλ₯ λΆκ΄΄ νμκ³Ό λ°λ¦¬ μ λμ μ μ΄νκΈ° μνμ¬ μμ λΆκ·Όμ jetμ μμΉμμΌ°λ€. νλ
μ€νμ ν΅νμ¬ μμ μ μμΉν jetμ λͺ¨λ μλ μμΌ μ λμ μ΄ ν¨κ³Όλ₯Ό νμΈνμλ€. λν κ³ μ±λ₯, μ μ λ ₯ ꡬλμ μνμ¬ jetμ κ°μμ λ°λ₯Έ μ λμ μ΄ μ±λ₯μ νκ°νμλ€. μμΉν΄μμ ν΅νμ¬ jetμ μμΉμ λ°λ₯Έ μ λμ μ΄ λ©μ»€λμ¦μ νμΈνκ³ μμΉμ λ°λΌ μ λμ μ΄λ₯Ό μνν κ²½μ° μλ₯ λΆκ΄΄ νμμ μ§μ°μν€κ³ λ°λ¦¬ μ λμ μ μ΄ν μ μμμ νμΈνμλ€. λν κ³ μμμμ μ λμ μ΄ κ°λ₯μ±μ νμΈνκΈ° μνμ¬ μ μμμμ μ λμ μ΄ μ λ΅μ κ³ μμμ νμ₯ μ μ©νμ¬ κ³ μμ λ체-λ κ° νΌν©νμμμλ ν¨κ³Όμ μΈ μ λμ μ΄ λ°©λ²μ ν΅νμ¬ κ³ λ°μκ°μ 곡λ ₯ μ±λ₯μ ν₯μ μν¬ μ μμμ νμΈνμλ€.
λ³Έ μ°κ΅¬μμ λμΆλ μ°κ΅¬ κ²°κ³Όλ μ λμ μ΄μ ν¨κ³Όμ μΈ λ₯λμ λμ μ΄ μμ€ν
μ μ€κ³ λ° λ¬΄μΈ μ ν¬κΈ° νμμ ν¬ν¨ν 3μ°¨μ λ κ° νμμ 곡λ ₯ μ±λ₯ ν₯μ λ°©μ μ립μ νμ©λ μ μμ κ²μ΄λ€.The present study deals with flow characteristics of synthetic jets for efficient flow control performance. It consists of two parts: flow characteristics of synthetic jets depending on exit configuration and flow control using synthetic jets over Blended Wing Body (BWB) configuration.
In first part, flow characteristics of synthetic jets have been computationally investigated for different exit configurations under a cross flow condition. The exit configuration of a synthetic jet substantially affects the process of vortex generation and evolution, which eventually determines the mechanism of jet momentum transport. Two types of exit configurations were considered: one is a conventional rectangular exit, and the other is a series of circular holes. The interactions of synthetic jets with a freestream were performed by analyzing the vortical structure characteristics. The effectiveness of flow control was evaluated by examining the behavior of the wall shear stress. It was observed that the circular exit provides better performance than the rectangular exit in terms of sustainable vortical structure and flow control capability. According to a hole gap and a hole diameter of circular exit, comparative studies were then conducted with all the other parameters fixed. Detailed computations reveal that the hole gap yields a much more significant effect on flow characteristics than the hole diameter, which turned out to be relatively minor. Based on the strength and the persistency of jet vortices, the circular exit with a suitable hole gap formed critical jet vortices that beneficially affected separation control. This indicates that the flow control performance of circular exit array could be remarkably improved by applying a suitable dimensionless hole parameter.
Based on the results of exit configuration, the second part deals with flow control strategy over BWB configuration. Flow structures were examined by analyzing the baseline characteristics of BWB configuration when synthetic jet was off. Based on the aerodynamic data and flow structure, a strategy for flow separation control on BWB configuration was established. Based on the aerodynamic data and flow structure, synthetic jet actuators were installed to prevent leading-edge stall at a relatively high angles of attack. All-actuators-on case and selective-actuators-on case were examined to find effective flow control method. Two types of exit locations are considered for analyzing flow mechanism: one is outboard array jets, and the other is inboard array jets. The interactions of synthetic jets with a free stream were performed by analyzing the vortical structure and the surface pressure characteristics. The effectiveness of flow control was evaluated by examining the aerodynamic coefficient and flow structures. As a result, the vortex breakdown point is moved toward the outboard section by synthetic jets, and the separation flow shows a stable structure. Based on the flow structure in overall speed rage, flow control strategy of low speed flight is applied to flow control of high speed flight. This shows effective flow control strategy applicable to all speed flight.
Through numerical analyses on flow characteristics of synthetic jets, it is observed that the synthetic jets under suitable actuating conditions beneficially change the local flow feature and vortex structure to bring a significant improvement of the wing aerodynamics acting on the three-dimensional aircraft configuration in the stall angle.Chapter I Introduction 1
1.1 Literature Review 1
1.1.1 Synthetic Jet 1
1.1.2 Piezoelectirically-driven Synthetic Jet 3
1.1.3 Lambda Wing Aerodynamics 4
1.1.4 Flow Separation on Lambda Wing Flight Mechanics 5
1.1.5 1303 UCAV Configuration 7
1.2 Objectives and Contributions 10
1.3 Organization of Thesis 11
Chapter II Numerical Approaches 12
2.1 Governing Equations 12
2.2 Turbulence Models 14
2.2.1 The Standard Menters k-Ο SST Model 14
2.2.2 The k-Ο SST Model (Menter et al., 2003) 18
2.2.3 SST-DES Model (Strelets et al., 2001) 19
2.2.4 Zonal SST-DES Model (Menter et al., 2003) 21
2.3 Pseudo-Compressibility Method 22
2.4 Transformation of the Incompressible Navier-Stokes Equations with Turbulence Model 27
2.5 Space Discritizaion Method 31
2.5.1 Differencing of Inviscid Flux Terms 31
2.5.2 Upwind Differencing Method 33
2.5.3 Low Dissipative Upwind Differencing Method 38
2.5.4 Higher Order Spatial Accuracy 39
2.6 Time Integration Method 41
2.6.1 Dual Time Stepping 42
2.6.2 Pseudo-Time Discretization 44
2.6.3 LU-SGS Scheme 47
2.7 Synthetic Jet Boundary Condition 50
Chapter III Flow Characteristics of Synthetic Jets 51
3.1 Two Types of Synthetic Jet Exit 51
3.2 Code Validation 53
3.3 Characteristics of Rectangular and Circular Exits 55
3.3.1 Flow Structures 55
3.3.2 Flow Control Effectiveness 58
3.4 Characteristics of Circular Exits Depending on Hole Parameter 60
3.4.1 Variation of Hole Gap 60
3.4.2 Variation of Hole Diameter 62
Chapter IV Active Flow Control of Wing 63
4.1 Experimental Reference 63
4.1.1 BWB Configuration 63
4.1.2 Experimental Setup 64
4.2 Baseline Analysis 65
4.2.1 Code Validation 65
4.2.2 Flow Characteristics of BWB Configuration 67
4.3 Flow Control of BWB Configuration 69
4.3.1 Flow Control Depending on Jet Location 69
4.3.2 Application of Flow Control in High Speed Flight 72
Conclusion 75
References 77Docto