Adaptive Winglet Design, Analysis and Optimisation of the Cant Angle for Enhanced MAV Performance

Similar documents
Mechanics of Flight. Warren F. Phillips. John Wiley & Sons, Inc. Professor Mechanical and Aerospace Engineering Utah State University WILEY

Aeroelastic Gust Response

Aero-Propulsive-Elastic Modeling Using OpenVSP

Fundamentals of Airplane Flight Mechanics

/ m U) β - r dr/dt=(n β / C) β+ (N r /C) r [8+8] (c) Effective angle of attack. [4+6+6]

Experimental Evaluation of Aerodynamics Characteristics of a Baseline Airfoil

Chapter 1 Lecture 2. Introduction 2. Topics. Chapter-1

ME 425: Aerodynamics

SIMULATION STUDIES OF MICRO AIR VEHICLE

Chapter 5 Performance analysis I Steady level flight (Lectures 17 to 20) Keywords: Steady level flight equations of motion, minimum power required,

INVESTIVATION OF LOW THRUST TO WEIGHT RATIO ROTATIONAL CAPACITY OF ASYMMETRIC MONO-WING CONFIGURATIONS

FLIGHT DYNAMICS. Robert F. Stengel. Princeton University Press Princeton and Oxford

Stability and Control

A Numerical Blade Element Approach to Estimating Propeller Flowfields

Biologically inspired sensor fusion for real-time wind gust estimation in autonomous UAV navigation

Fullscale Windtunnel Investigation of Actuator Effectiveness during Stationary Flight within the Entire Flight Envelope of a Tiltwing MAV

Royal Aeronautical Society 2016 Applied Aerodynamics Conference Tuesday 19 th Thursday 21 st July Science Centre, Bristol, UK

Calibration Methods for an Aerolab 375 Sting Balance to be used in Wind Tunnel Testing

Stability and Control Analysis in Twin-Boom Vertical Stabilizer Unmanned Aerial Vehicle (UAV)

Experimental Aircraft Parameter Estimation

Design and modelling of an airship station holding controller for low cost satellite operations

Optimization Framework for Design of Morphing Wings

Study. Aerodynamics. Small UAV. AVL Software

MODULAR AEROPLANE SYSTEM. A CONCEPT AND INITIAL INVESTIGATION

Localizer Hold Autopilot

MAV Unsteady Characteristics in-flight Measurement with the Help of SmartAP Autopilot

What is flight dynamics? AE540: Flight Dynamics and Control I. What is flight control? Is the study of aircraft motion and its characteristics.

Introduction to Flight Dynamics

Flight Dynamics, Simulation, and Control

AEROSPACE ENGINEERING

Introduction to Flight

Evaluation of the Drag Reduction Potential and Static Stability Changes of C-130 Aft Body Strakes

Configuration Aerodynamics

Flight Dynamics and Control

Performance. 5. More Aerodynamic Considerations

PRINCIPLES OF FLIGHT

The Study on Re Effect Correction for Laminar Wing with High Lift

Aircraft stability and control Prof: A. K. Ghosh Dept of Aerospace Engineering Indian Institute of Technology Kanpur

UNIVERSITY OF CALGARY INFLUENCE OF GROUND EFFECTS ON BODY FORCES FOR BI-COPTER UAV. Daniel Norton A THESIS

Chapter 5 Wing design - selection of wing parameters 2 Lecture 20 Topics

ν δ - 1 -

NUMERICAL OPTIMIZATION OF THE SHAPE OF A HOLLOW PROJECTILE

Experimental Aerodynamics. Experimental Aerodynamics

Given the water behaves as shown above, which direction will the cylinder rotate?

AE Stability and Control of Aerospace Vehicles

German Aerospace Center (DLR)

ANALYSIS OF AUTOPILOT SYSTEM BASED ON BANK ANGLE OF SMALL UAV

Pitch Control of Flight System using Dynamic Inversion and PID Controller

CFD COMPUTATION OF THE GROUND EFFECT ON AIRPLANE WITH HIGH ASPECT RATIO WING

Aircraft Design I Tail loads

Autonomous Robotic Vehicles

Stability and Control Some Characteristics of Lifting Surfaces, and Pitch-Moments

Mathematical Modeling of the Flow behind Propeller

Aerodynamic Design of VTOL MAV

Flight and Orbital Mechanics. Exams

Active Guidance for a Finless Rocket using Neuroevolution

A SIMPLIFIED ANALYSIS OF NONLINEAR LONGITUDINAL DYNAMICS AND CONCEPTUAL CONTROL SYSTEM DESIGN

FLOW ANALYSIS AND DETERMINATION OF DRAG FORCES FOR SPIKES OF CROPS. S. Kırmacı and M. Pakdemirli

PROGRESS IN THE PREDICTION OF AEROSERVOELASTIC INSTABILITIES ON LARGE CIVIL TRANSPORT AIRCRAFT

The future of non-linear modelling of aeroelastic gust interaction

Wind Tunnel Study of a Large Aerostat, CFD Validation

Estimation of Wind Velocity on Flexible Unmanned Aerial Vehicle Without Aircraft Parameters

AERODYNAMIC PERFORMANCE OF A REMOTELY PILOTED VEHICLE

Optimum Design of a PID Controller for the Adaptive Torsion Wing Using GA

MODELING OF SPIN MODES OF SUPERSONIC AIRCRAFT IN HORIZONTAL WIND TUNNEL

Dynamic Response of an Aircraft to Atmospheric Turbulence Cissy Thomas Civil Engineering Dept, M.G university

Trajectory Tracking of a Near-Surface Torpedo using Numerical Methods

ACTIVE SEPARATION CONTROL ON A SLATLESS 2D HIGH-LIFT WING SECTION

Mathematical Modelling and Dynamics Analysis of Flat Multirotor Configurations

Efficient Modelling of a Nonlinear Gust Loads Process for Uncertainty Quantification of Highly Flexible Aircraft

Simulation of UAV Systems P. Kaňovský, L. Smrcek, C. Goodchild

A First Order Model of a Variable Camber Wing for a Civil Passenger Aircraft

Dynamics and Control Preliminary Examination Topics

MASTER THESIS PRESENTATION

Drag reduction in a class 8 truck - scaled down model

Figure 1 UAV Geometry Base Case Design

A Numerical Study of Circulation Control on a Flapless UAV

Design of a Morphing Wing : Modeling and Experiments

Experimental Study on Flow Control Characteristics of Synthetic Jets over a Blended Wing Body Configuration

Modeling of a Small Unmanned Aerial Vehicle

THEORETICAL AND EXPERIMENTAL INVESTIGATION OF ENERGY EXTRACTION FROM ATMOSPHERIC TURBULENCE

Aircraft Stability & Control

DEPARTMENT OF AEROSPACE ENGINEERING, IIT MADRAS M.Tech. Curriculum

Analyses of Diamond - Shaped and Circular Arc Airfoils in Supersonic Wind Tunnel Airflows

Introduction to Atmospheric Flight. Dr. Guven Aerospace Engineer (P.hD)

University of Huddersfield Repository

1082. Computational study on aerodynamic characteristics of a flying wing MAV

EXPERIMENTAL INVESTIGATION OF THE DYNAMIC STABILITY DERIVATIVES FOR A FIGHTER MODEL

Turn Performance of an Air-Breathing Hypersonic Vehicle

Real-time trajectory generation technique for dynamic soaring UAVs

The Fundamentals of Classic Style Skydiving by Vladimir Milosavljevic, assisted by Tamara Koyn

FLIGHT DYNAMICS ANALYSIS AND BASIC STABILIZATION STUDY IN EARLY DESIGN STAGES OF THE SAGITTA DEMONSTRATOR UAV

MODELING OF A SMALL UNMANNED AERIAL VEHICLE

AM25 UNMANNED AIR VEHICLE FLIGHT CONTROL

Numerical analysis of the influence of particular autogyro parts on the aerodynamic forces

Lecture No. # 09. (Refer Slide Time: 01:00)

COMPUTATIONAL SIMULATION OF THE FLOW PAST AN AIRFOIL FOR AN UNMANNED AERIAL VEHICLE

Balance of Moments for Hypersonic Vehicles

The Analysis of Dispersion for Trajectories of Fire-extinguishing Rocket

JAA Administrative & Guidance Material Section Five: Licensing, Part Two: Procedures

Transcription:

Adaptive Winglet Design, Analysis and Optimisation of the Cant Angle for Enhanced MAV Performance Chen-Ming Kuo and Christian Boller University of Saarland, Materials Science & Technology Dept. Chair of Nondestructive Testing & Quality Assurance Campus E3.1, 66123 Saarbrücken, Germany ABSTRACT Adaptive air vehicle structures are an interesting option for enhancing an air vehicle s performance. This has been shown to be true even for MAV where a variety of solutions with regard to adaptive wings and tails have been presented so far in the past. Within the paper to be presented here an adaptive winglet for a MAV of 4cm in span and 25cm in length will be described. This is the size of a bird where bio-inspiration has been a good source for generating the adaptive winglet idea. Based on a modular MAV design and a flexible CAD model being already available, the adaptive winglet with variable cant angle could be simulated, designed, realised and validated. The CFD simulations of the MAV with winglet were done for various flight conditions and represented by factors such as best aerodynamic efficiency, stability and manoeuvrability. Optimum winglet angle search for best performance was done by using Genetic Algorithms. In order to expand the limited data points without doing too much CFD simulation, a new technique of grey prediction (using the rolling model) has been applied. Results predicted with this procedure are rather close to CFD results, with slightly less than 1% error in general and the optimum winglet angle to be determined very much in accordance to reality. With all the data from different simulations and algorithms used a working prototype with the mechanism for an active adaptive winglet was realised and its performance shown in hardware. 1 INTRODUCTION Most of the commercial long range aircraft has installed winglet to decrease the induce drag to save more fuel, this feature can be also found on the bird. Bird use its feather at wingtip as multiple winglet, which can be seen Fig. 1. Each feather has different angle respect to the wing, and they are passively adapted to the different flight conditions, which is different from the fixed angle winglet in the conventional aircraft (only designed for cruise). Such adaptive winglet feature can be studied and implemented on the platform MAV to evaluate its performance and usefulness. All parts of this document have their own style (section headings, subsection headings, text, captions, etc.). You can select a style for your text, by selecting the text and then selecting the appropriate style in the style bar (left of the font type and size). Regular text should have the style Text. The EMAV 29 preserves the right to adjust the Email address: chen.kuo@mx.uni-saarland.de formatting of papers if necessary. However, passive adaptive multiple winglet requires deep understanding of Fluid Structure Interaction, which is very time consuming and requires large amount of computational resources. In order to avoid the complexity of FSI, the problem is simplified to active control winglet (ie, no FSI effect). Fig. 1 A bird s wing during flight.[1] Instead of having multiple winglets, one winglet on each side of the wing is used (like conventional aircraft), and angle of the winglet can be varied. Also, this setup can be the first step to understand the effect of the adaptive winglet. 2 MAV TEST PLATFORM The test platform MAV has 4cm wing span with length of 25cm, detail dimension drawing can be seen in Fig. 2. The platform is stable with long endurance, which has been use to demonstrate and evaluate of different adaptive structures before [1],[2],[3]. therefore, it is very suitable platform for the study in this paper. The MAV weights 2g (the test version), with flight speed of 8m/s. It has unique of vector thrust propulsion unit, allows the low energy consumption for entire flight. Fig. 2. The dimension of the MAV. Note: all units are in mm. 3 DEVELOPMENT PROCEDURES Since the MAV is quite a new field, therefore there is no

actual research about the winglet size and angle, therefore, everything need to start from ground in this case. There are varies adaptive structure has been design on the platform MAV; therefore, the adaptive winglet design must be able to be independently implemented on platform and integrate with other adaptive structures. For this reason, the adaptive winglet in with integration to platform is shown in Fig. 3 Fig. 3. Left, platform MAV with winglet (iso view). Right, back-view of the MAV with winglet. However, instead simulate all the different angle of winglet, only few are selected to speed up the design and analysis process, and selected one are: -5,-3,,2,45 and 65 degree, the CAD model of each can be seen in Fig. 4 Fig. 6. The aeroelasticity test of the MAV in wind tunnel. Note. The marker system are provided by Fraunhofer ITB Germany. For the fair test, all the mesh for CFD are kept constant in all simulation, boundary layer assume to be <15mm (by the experience). Hybrid mesh was used for boundary layer and air around it to reduce the computational resources,, and typically 2 million cell were in the mesh. Fig. 4. CAD model of different winglet angle, from the top left to bottom right are:-5,-3,,2,45,65 degree. Because aerodynamic performance is not the only factor consider in this paper, therefore the simulation setup must consider varies different flight condition in order to evaluate factor such as stability and maneuverability [4]. CFD simulation assume the flow speed of 12m/s due to the propeller plus its own flight speed (ie the Re number is at 192,). This condition has been proved in wind tunnel test in DLR in Göttingen. Since the MAV geometry is complex, the use of K ω model become difficult and required high computational resources in storing the detail of boundary layer mesh, also, the simulation of the MAV flight is mostly with-in the stall region, therefore, standard K εmodel is selected for this study. The results has also be tested in the wind tunnel in DLR for aeroealsticity, the accuracy is of Fluid solid interaction simulation are well fit in around 5%, which shows the reliability of the CFD model. (please note, the model is not suitable for testing in stall region, which all the experimental and simulation are all carried out in pre stall region) Fig. 5. Wind tunnel test model Fig. 7. Left, mesh of the flow region. Right, mesh around the MAV. The overall design and development process block diagram can be seen in Fig. 8. Fig. 8. Block diagram of the design and development process. 4 NUMERICAL METHOD Genetic Algorithm Genetic algorithm (GA) is a computational method for searching the solution of the optimal point. Traditionally, solution are represented in binary as strings of and 1, therefore, the input value (analogue) in this case must convert to binary. The algorithm starts from some randomly generated Parents generation, and fitness of every individual is evaluated, multiple individuals are stochastically selected from the current population, and modified (cross over and some randomly mutated). In this case the input value is the angle of winglet, since the range is between to 36 degree, therefore, 1 digit

binary is selected as gene. In order to make sure there is optimal solution before end of generations, therefore, 1 generations are set. Biologically, mutation only sometimes generate better offspring, therefore, the rate is set to be 1%, and cross rate is set to be 6%. Base on the available data point, functions are roughly estimated, and then G.A uses this function to search the maximum and minimum point (aerodynamic efficiency, stability and maneuverability). Grey prediction Grey predication is treating system as a grey system. In grey system theory, a dynamic model with a group of differential equations called grey differential model. The grey derivative and grey differential equation are defined and proposed in order to build a grey model.[5] There are many different type of grey model, and common one are GM(1,N) and GM(1,1) model, Since data prediction is required, therefore GM(1,1) model should be selected, and by definition, at least four set of data is needed; in this case, the input is angle of the winglet, output is the stability and maneuverability, therefore, 6 data point can be collected (which satisfy the condition of using grey model). Equation (1.1) and (1.2) is the solution for GM(1,1) model. ) () b ak b x( K + 1) = x(1) e +, a a () (1) (1) xˆˆˆk ( + 1) = x( K + 1) x( K ) [1] 5 RESULTS CFD simulated results The first simulated results include the winglet cant angle of, 2, 45, 65, -3, and -5. Each model has go tough series of CFD simulation for different flight conditions, results of longitudinal and lateral stability are compared with the MAV without any winglet. All simulated results are shown from Fig. 9 to Fig. 12. C h a n g e i n U v e l o c i t y ( m / s ) 2 1. 5 1. 5 -. 5-1 L o n g i t u d i n a l s t a b i l i t y o f + 2 U v e l o c i t y i n p u t R i g i d w i n g d e g r e e ( W i n g l e t ) - 5 d e g r e e - 1. 5 5 1 1 5 2 2 5 3 Fig. 9. Longitudinal stability results of the MAV (change in U velocity) Longitudinal All three different output results shows the most stable configuration is where the cant angle is equal to, and most unstable configuration is -5. Note: these results are only base on the simulated cases, which does not mean the definite results. C h a n g e i n W v e l o c i t y ( m / s ). 3. 2. 1 -. 1 -. 2 -. 3 L o n g i t u d i n a l s t a b i l i t y o f c h a n g e i n W v e l o c i t y r e s p o n s t o + 2 m / s i n U R i g i d W i n g d e g r e e - 5 d e g r e e -. 4 5 1 1 5 2 2 5 3 Fig. 1. Longitudinal stability results of the MAV (change in W velocity) C h n a g e i n b e t a ( r a d ). 1. 8. 6. 4. 2 L a t e r a l s t a b i l i t y o f b e t a i n r e s p o n s e o f +. 8 7 ( 5 d e g r e e ) i n s i d e s l i p R i g i d w i n g d e g r e e - -. 2. 1. 2. 3. 4. 5. 6. 7. 8. 9 1 C h a n g e i n r ( r a d / s ) 2. 5 1. 5. 5 Fig. 11. Lateral stability results of the MAV (change in β) 2 1 L a t e r a l s t a b i l i t y o f r i n r e s p o n s e o f +. 8 7 b e t a ( 5 d e g r e e ) R i g i d w i n g d e g r e e - 5 d e g r e e -. 5. 5 1 1. 5 Fig. 12. Lateral stability results of the MAV (change in r) Laterally Simulated results in all cases shows the additional winglet cases damping ratio to drop, and MAV response to gust faster (but with overshoot). This is very logic, since winglet (doesn t matter which angle it is at) creates additional surfaces area in XZ plan (body coordinate system of the aircraft), and these additional surfaces cases additional forces and moment to be generated during lateral disturbance, in theory this should increase the speed of reaction, however, because the winglet in this experiment was located slightly in front of the C.G (due to the Zimmerman profile and vector thrust propulsion unit), therefore, the additional forces is resulting decreasing the overall damping ratio of the motion (speed up the response). This results also agree with Corneil s work in early 8s [6]. However, the with this increase in the response speed to gust, means decrease maneuverability, and from Fig. 11 and Fig. 12 shows the best maneuverability occur with 65 winglet configuration, where the response is slowest (if

consider MAV with winglet configuration only). Genetic algorithm search for best performance of the winglet angle Since data obtain from the CFD simulation are limited, and with these limited data, one can only identify the best results from select cases. However, the best results may not be in those exact cases (ie, best longitudinal stability may occur in 32 degree, which was not the simulated case). In order to solve this problem, genetic algorithm model was written for search the best aerodynamic performance, stability and maneuverability. The research results shows from Fig. 13 to Fig. 15, and compiled results table is shown at Table 1. M i n i m u m v a l u e o f t h e f u n c t i o n G e n e t i c A l g o r i t h m s e a r c h f o r b e s t C L / C D i G e r n e r a t o n s Fig. 13 G.M search of minimum value of the function for CL/CD m i n v a l u e o f f u n c t i o n 7. 2 1 7. 2 9 7. 2 8 7. 2 7 7. 2 6 7. 2 5 7. 2 4 7. 2 3 7. 2 2 7. 2 1 G e n e t i c a l g o r i t h m s e a r c h f o r b e s t l o n g i t u d i n a l s t a b i l i t y i 7. 2 G e n e r a t o n s Fig. 14 G.M search of minimum value of the function for Longitudinal stability (base on the damping ratio of the motion) m i n v a l u e o f t h e f u n c t i o n G e n e t i c a l g o r i t h m s e a r c h f o r t h e b e s t l a t e r a l s t a b i l i t y i G e n e r a t o n s Fig. 15. G.M search of minimum value of the function for lateral stability (base on the damping ratio of the motion) CL/CD Longitudinal Lateral stability stability Max (at degree 35.6452-39.638 of winglet) Min -41.16-42 65 Table 1. Results of G.M search for best and worst performance of the variable angle winglet angle. Note: min stability represent best maneuverability. The results from the G.A clearly shows some data that was not visible by just looking at selected CFD cases, and these information can be used for further autopilot design data base or pilot. Using combination of Grey prediction and Genetic algorithm for searching best performance G.A model is base on the already know data point and functions to search the best results, however, more data point it has, more accurate the function can be, hence, more accurate the G.A results will be. As mentioned before, Grey prediction (G.P) uses the numbers of exciting data to predict the next set of data, which is completed different to G.A. In this project, rolling model method is used, and results is shown at table 2 Angle of winglet Longitudinal damping Lateral damping ratio ratio -5.176.53689-3.24.648.1378.5594 2.9.5275 45.787.52334 65.9411.57812 85.174.4761 15.1163.4554 125.995.443 145.983.417 165.97.397 185.958.3717 Table 2. The results of grey prediction of the damping ratio for both longitudinal and lateral motion. Note: black shows CFD results, and orange shows the G.P value. Note: 18 degree is not the same as degree, see figure.2 for the orientation angle of the winglet. Results from the G.P are later used in the G.A modeling. Even the data now is bigger; solution still converged before it gets to the default number of generation (1 in this project), results are shown in Fig. 16,Fig. 17 and compiled results in Table 3. Even though the longitudinal results from Table 3 and Table 1 shows very similar, there is still have some slightly variation. However, the story is completed different in the lateral mode; there is 5 degree different for the max stability, but completely different story about the minimum stability. The main reason for such different is because before G.P modeling, the data point is only up to 65 degree, and according to the data collected, which is not enough for G.M to solve the case, therefore the search stop at 65 degree. With G.P model, the data expanse to 185 degree, and with sufficient data point, much better G.A search can be preformed. m i n v a l u e o f t h e f u n c t i o n m i x t u r e o f G r e y P r e d i c t i o n a n d G e n t i c A l g o r i t h m f o r l o n g i t u d i n a l m o t i o n g e n e r a t i o n

Fig. 16 Mixture of G.P and G.M search of minimum value of the function for longitudinal stability (base on the damping ratio of the motion) M i n v a l u e o f f u n c t i o n m i x t u r e o f G r e y P r e d i c t i o n a n d G e n t i c A l g o r i t h m f o r l a t e r a l m o t i o n G e n e r a t i o n Fig. 17. Mixture of G.P and G.M search of minimum value of the function for lateral stability (base on the damping ratio of the motion) Longitudinal stability Lateral stability Max -3.158-34.346 Min -43 185.1678 Table 3. Results of mixture of G.P and G.M search for best and worst performance of the variable angle winglet angle. Note: min stability represent best maneuverability. Aerodynamically, the best efficient shows at 35.65 degree, which if recall Fig. 1, bird s winglet angle is not at 9 degree during the steady flight. In fact, when eagle is during the steady flight, the winglet angle is around 3 to 4 degree [7], which is in the range results obtain from this project. Looking stability/maneuverability, longitudinally, the best stability at degree and best maneuverability is at round -42 to -43 degree. Bird s winglet can not go to negative degree, since it is only control passively, but if consider the shape of wing during when bird during dive to attack on its target, the wing is rather at M shape [8]. This M shape decreases the lift coefficient, and vortex center move more toward to the body side (where the weight is), this similar effect can be seen when the winglet is at negative angle (Fig. 18), and therefore, it makes the bird and MAV easier to move in the longitudinal direction. maneuverability occur at the 187 degree. The reason for this effect is also to do with where the lift location and value. When lift is closer toward to the body, the moment for the lateral motion decreased when the same disturbance occurs, therefore the MAV resist the change. All the results in the study indicate that all the best performance of MAV occur at different angle of winglet, therefore, for the in order to achieve most efficient flight, active control of winglet is required, and results from this study can be used for future autopilot design. One other discovery in this study was that even use asymmetric variable angle winglet for maneuver is not efficient enough. Consider MAV with left side of wing has winglet of 9 degree (flat), and the right side of degree, then the lift one the left is higher, which cause the rolling moment to the right, but side down wash on the right side is lower (because of the winglet), this will make the yawing moment to the left, therefore it is in conflict with rolling moment created. Further more, when MAV is turn left with this configuration, the right side winglet is acting like vertical tail, which will generate side force to the right to resist the rolling moment. These motion can be seen in Fig. 19, and was also confirm with Bourdin s [9] and Corneil s [6] work. Fig. 19. Asymmertic winglet MAV during the turn. (front view at right) 6 HARDWARE PROTOTYPING Since the individual moment of winglet does not have any benefit (can see from Fig. 19), therefore, 2 winglet must be able to varies its angle together. For this requirement, only one servo is needed. The condition is very similar to the Ref[1], therefore only small modification is needed form the original design. Fig. 2. The deflection of the winglet on the MAV. Note the mechanical linkage. Fig. 18. The stream line of MAV with different angle of winglet. Note: the location of the vortex center is clearly different. Laterally, results of CFD simulation shows the configuration without winglet has best stability, reason has been discussed before. However, if looking at winglet configuration, the best stability occurs at -34 degree from the G.A, and -39 degree with G.P & G.A modeling. Max 7 CONCLUSION Study in this project shows the how the with a simple winglet configuration, the overall performance of aerodynamic efficiency, stability and maneuverability can be changed. Optimal angle of aerodynamic, stability and maneuverability performance has been identify with use either CFD data only, G.A only, and mixture of G.P and

G.A. Traditional design and analysis process is time consuming, however, using limited data point from CFD, using mixture of G.P rolling model and G.A generating more data point, and search the optimal point is fast and more efficient. Optimal angle for aerodynamic performance is around 35 degree. Longitudinally, most stable at to -5 degree, and most maneuverable at -42 to -43 degree. Laterally, most stable at -34 to-39 degree, and most maneuverable at 185 degree. These results pattern also confirm with the natural bird s flight. 8 FUTURE WORK This paper shows the optimal angle for MAV performance, these data can be given to the autopilot design or flight programming. Second step, with optimal angle and aerodynamic data known for the max CL/CD, therefore, passive winglet development can be possible. Lastly, in order to get even more bio-inspired, both active and passive multiple wing let can be design and develop for the future. REFERENCE [1] Kuo C-M, C Boller and N Qin, 28: Modular design of a Micro air vehicle for demonstration of adaptive structure performance ; Proc. of European Workshop on Micro Aerial Vehicles, Braunschweig/Germany [2] Kuo C-M, C Boller and N Qin, 26: Adaptive MAV interns of aerodynamic, mission capability and energy efficiency ; Proc. of 2 nd European Workshop on Micro Aerial Vehicles, Braunschweig/Germany [3] Kuo C-M, C Boller and N Qin, 27: Enhancing MAV Stability in Gusty Wind by Wing Flexibility- Analyses and Flight Tests ; 22 nd International UAV Conference, Bristol, [4] Barnes W. McCormick. Aerodynamics Aeronautics and Flight Mechanics. John Wiley & Son, Inc, 2 nd edition [5] David K. W.Ng, Grey system and grey relational model. ACM SIGICE Bulletin, Voluume 2, issue 2, Oct 1994. ISSN 893-2875 [6] Cornelis P. van Dam, Bruce J. Holmes and Calvin Pitts, Effect of Winglets on Performance and Handling Qualities of General Aviation Aircraft. Journal of Aircraft 1981. 21-8669 vol.18 no.7 (587-591) [7] Taronga zoo s wedge tail eagle takes flight in Sydney. Web accessed Nov/28. address: http://www.zimbio.com/pictures/tk6yjeb39jy/ Taronga+Zoo+Wedge+Tail+Eagle+Takes+Flight/mA5XoADhVZ [8] DavidMixner.com Live From Turkey Hollow. Web accessed Jun/28. address: http://www.davidmixner.com/28/4/jonathanstolle.html [9] P.Bourdin, A.Gatto, and M.I. Friswell. The Application of Variable Cant angle winglets for Morphing aircraft control. 24 th Applied Aerodynamic Conference. June 26. San Francisco, US.