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PROPELLER LOCATIONS STUDY ON DELTA-WINGED UNMANNED AERIAL VEHICLE (UAV) MODEL KHUSHAIRI AMRI BIN KASIM A thesis submitted in fulfilment of the requirements for the award of the degree of Master of Philosophy Faculty of Mechanical Engineering Universiti Teknologi Malaysia MARCH 2017

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Page 1: PROPELLER LOCATIONS STUDY ON DELTA-WINGED UNMANNED ...eprints.utm.my/id/eprint/78655/1/KhushairiAmriKasimMFKM2017.pdf · Akhir sekali, kesan penggunaan kipas terhadap aliran pusaran

PROPELLER LOCATIONS STUDY ON DELTA-WINGED UNMANNED

AERIAL VEHICLE (UAV) MODEL

KHUSHAIRI AMRI BIN KASIM

A thesis submitted in fulfilment of the

requirements for the award of the degree of

Master of Philosophy

Faculty of Mechanical Engineering

Universiti Teknologi Malaysia

MARCH 2017

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iii

Specially dedicated to my supportive and lovely parents,

siblings and friends for always being at my side.

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iv

ACKNOWLEDGEMENT

First and above all, I praise Allah S.W.T for providing me this opportunity

and granting me the capability to proceed successfully. This thesis appears in its

current form due to the assistance and guidance of several people. I would therefore

like to offer my sincere thanks to all of them.

Firstly, I would like to express my sincere gratitude to my supervisor Dr.

Shabudin bin Mat for the continuous support of my Master study and related

research, for his patience, motivation, and immense knowledge. His guidance helped

me in all the time of research and writing of this thesis. I also would like to thank

my co-supervisor Dr. Iskandar Shah bin Ishak for his constant support availability

and constructive suggestion, which were determined for the accomplishment of the

work presented in this thesis.

Besides my advisor, I would like to thank the rest of my thesis committee:

Dr. Rizal Effendy Mohd Nasir and Assoc. Prof. Dr. Syahrullail bin Samion for their

insightful comments and encouragement, but also for their insight which encouraged

me to widen my research from various perspectives.

My sincere thanks also to the technicians of the UTM Aerolab for their help

in offering me the resources in running the research. Without their precious supports

and guides, it would not be possible to finish this research.

Finally, I must express my very profound gratitude to my parents and to my

friends for providing me with unfailing support and continuous encouragement

throughout my years of study and through the process of writing this thesis. This

accomplishment would not have been possible without them.

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v

ABSTRACT

Delta wing design is being used in aircraft to obtain high manoeuvre properties.

The flow above the delta wing is complicated and dominated by a very complex vortex

structure. This research investigates the effects of the propeller locations on the

aerodynamic characteristics above a generic 55° sharp-edged non-slender delta wing

Unmanned Aerial Vehicle (UAV) model. This research was performed by an

experimental method. The experiments were conducted in a closed circuit Universiti

Teknologi Malaysia-Low Speed Tunnel (UTM-LST) wind tunnel at wind speed of 20

m/s and 25 m/s respectively. In this project, the propeller was located at three different

locations at front, middle and rear of the wing. The experimental data highlights an

impact of propeller locations on lift, drag, pitching moment and vortex characteristic

of the UAV model. Rear propeller configuration recorded the highest lift generation.

Meanwhile, middle propeller configuration has the highest drag with increment by 2%

to 15%. The results also show that the propeller advance ratio plays important roles in

development of the primary vortex above the delta-winged model. The higher

propeller advance ratio would decrease the development of the vortex on the wing,

consequently limiting the lift generation and stall condition in which are

disadvantageous for aircraft aerodynamic characteristics. The lift coefficients decrease

by 7% when the propeller advance ratio is increased from 0.98 to 1.20. Lastly, suction

effect from the propeller has improved the vortex properties better than blowing

mechanism in which is beneficial for the delta-winged UAV propeller selection.

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vi

ABSTRAK

Penggunaan reka bentuk sayap delta diaplikasikan pada pesawat bagi

memperoleh olah gerak yang tinggi. Penggunaan sayap delta ini dapat dimanfaatkan

dengan penghasilan daya angkatan yang lebih baik berbanding dengan reka bentuk

pesawat konvensional. Walau bagaimanapun, aliran udara di atas permukaan sayap

delta ini sangat kompleks kerana reka bentuk ini mempunyai aliran pusaran yang

terhasil di sisi sayap. Oleh itu, kajian ini dibuat bagi mengenal pasti kesan lokasi kipas

yang diletakkan pada model Pesawat Udara Tanpa Pemandu (UAV) dari segi aspek

aerodinamik dan corak perubahan aliran pusaran di atas permukaan sayap delta. Model

UAV yang digunakan dalam kajian ini merupakan sayap delta 55° bersisi tajam.

Kajian dijalankan secara eksperimen menggunakan terowong angin litar tertutup

Universiti Teknologi Malaysia-Low Speed Tunnel (UTM-LST) pada kelajuan angin

20 m/s dan 25 m/s. Posisi kipas diletakkan di tiga tempat berbeza iaitu di hadapan,

tengah dan belakang model. Hasil dapatan kajian difokuskan terhadap kesan lokasi

kipas terhadap daya angkatan, daya heretan, momen anggulan dan ciri vorteks. Data

daripada eksperimen mendapati pemasangan kipas terhadap model UAV

mempengaruhi daya angkatan, daya heretan dan momen anggulan model pesawat.

Kipas yang dipasang di belakang model mencatatkan nilai pekali daya angkat yang

tertinggi. Manakala kipas yang dipasang di tengah model mencatatkan daya heretan

yang tertinggi dengan peningkatan sebanyak 2% hingga 15%. Hasil dapatan kajian

juga menunjukkan bahawa nisbah mara kipas memainkan peranan penting dalam

pembentukan aliran pusaran di atas sayap delta. Nisbah mara kipas yang tinggi akan

mengurangkan pembentukan aliran pusaran di atas sayap delta sekaligus mengehadkan

penghasilan daya angkatan dan pendakian pesawat. Pekali daya angkat didapati

berkurangan sebanyak 7% apabila nisbah mara kipas dinaikkan dari 0.98 ke 1.20.

Akhir sekali, kesan penggunaan kipas terhadap aliran pusaran menunjukkan bahawa

mekanisme sedutan memberikan kesan yang lebih ketara berbanding dengan

mekanisme tiupan.

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TABLE OF CONTENTS

CHAPTER TITLE PAGE

DECLARATION ii

DEDICATION iii

ACKNOWLEDGEMENT iv

ABSTRACT v

ABSTRAK vi

TABLE OF CONTENTS vii

LIST OF TABLES x

LIST OF FIGURES xi

LIST OF SYMBOLS xv

LIST OF APPENDICES xvii

1 INTRODUCTION 1

1.1 Background of the Study 1

1.2 Delta Winged UAV 5

1.3 Research Objectives 7

1.4 Scope of Study 7

1.5 Significant of Studies 8

2 LITERATURE REVIEW 9

2.1 Why Delta Wing 9

2.2 Delta Wing Flow Topology 11

2.3 Non-Slender Delta Wing Flow Topology 17

2.4 Influences of Reynolds Number on Non-Slender Delta

Wing

22

2.5 Effects of Angle of Attack on Non-Slender Delta Wing 28

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2.6 Vortex Breakdown on Non-Slender Delta Wing 31

2.7 Delta Winged UAV Flow Topology 32

2.8 Delta Wing with Propeller Configuration 35

2.9 Delta-Winged UAV with Propeller Configuration 39

2.10 Unresolved Issues in Delta Wing Aerodynamics 51

3 METHODOLOGY 52

3.1 Research Design 52

3.2 UAV Wind Tunnel Model Design 54

3.3 Model Specification 57

3.4 Wind Tunnel Testing 61

3.5 Electrical Motor System 65

3.6 Propeller 66

3.7 Data Collection 66

3.8 Reynolds Number Calculation 70

3.9 Balance Data and Pressure Coefficient Calculation 71

3.9.1 Coefficient of Lift, CL 72

3.9.2 Coefficient of Drag, CD 72

3.9.3 Coefficient of Pitching Moment, CM 73

3.9.4 Coefficient of Pressure, CP 73

3.10 Data Correction Analysis 74

3.10.1 Solid Blockage 76

3.10.2 Wake Blockage 77

3.10.3 Total Blockage and Data Correction 79

3.11 Propeller Advance Ratio (J) 80

3.12 Data Presentations 81

4 RESULTS AND DISCUSSIONS 82

4.1 Repeatability Test 82

4.2 Results: Steady Balance 84

4.2.1 Effects of Reynolds Number (Clean Wing

Configuration)

84

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4.2.2 Effects of Propeller Advance Ratio, J

(Propeller Configurations)

87

4.2.3 Effects of Propeller Locations 93

4.3 Results: Surface Pressure Measurement 98

4.3.1 Effects of Reynolds Number on Pressure

Distribution

98

4.3.2 Effects of Propeller Advance Ratio, J on

Pressure Distribution

100

4.3.3 Effects of Propeller Locations on Pressure

Distribution

102

4.3.4 General Overview on Propeller Effects on

Vortex

111

4.5 Surface Pressure Contour 111

5 CONCLUSIONS AND RECOMMENDATIONS 117

5.1 Conclusions 117

5.2 Recommendations 119

REFERENCES 120

Appendices A-D 129-154

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x

LIST OF TABLES

TABLE NO. TITLE PAGE

1.1 Classification of UAVs by EUROVS 3

2.1 Comparison between tractor, pusher and middle propeller

configurations

50

3.1 Experiment set of the delta winged UAV model 64

3.2 Parameter of the model and correction factors for data

correction

76

3.3 Value of J in the experiments 80

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xi

LIST OF FIGURES

FIGURE NO. TITLE PAGE

1.1 Robo-fly UAV 2

1.2 LA100 UAV 4

1.3 Delta wing configurations 5

1.4 Several examples of delta winged UAVs 6

2.1 SYMDEL 1 10

2.2 Shear layer and leading-edge vortices above a delta wing 12

2.3 Leading edge flow structure on a delta wing 13

2.4 Lift on a delta wing 13

2.5 Internal structure of primary vortex 14

2.6 Main features flow with leading edge separation and

vortex sheet

16

2.7 Dual vortex structure formation on Λ=50° sweep delta

wing

17

2.8 Sketch of dual vortex mechanism 18

2.9 Dual vortex formation for 45° sweep delta wing 19

2.10 Effects of sweep angle toward vortex properties 20

2.11 Detachment of the primary vortex based on sweep angles 21

2.12 Effect of Reynolds number on vortex above non-slender

delta wing

22

2.13 Primary vortex location with Reynolds number from

several experiments

24

2.14 Primary vortex location with Reynolds number 24

2.15 Reynolds number effects on primary and shadow vortices

above non-slender delta wing

25

2.16 Effects of Reynolds number on dual vortex structure 26

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xii

2.17 Oil flow pattern of non-slender delta wing at Reynolds

number of 200,000

27

2.18 Effects angle of attack on vortex formation at Reynolds

number of 8,700

28

2.19 Vortex distance from wing at angle of attack 5° and 10° 29

2.20 Effects of angle of attack on vortex distance from wing

surface

29

2.21 Effect of angle of attack on vortex above non-slender

delta wing

30

2.22 Effects of angle of attack on surface flow pattern 31

2.23 Vortex breakdown on non-slender delta wing 32

2.24 Flow on 55° delta wing with different leading-edge radius 33

2.25 Flows on delta winged UAV with/without centerbody 33

2.26 Flow visualization studies over the upper surface of the

half-span 1303 UAV model at Re = 3.5 × 104

34

2.27 Surface flow field of Boeing 1301 UCAV 35

2.28 Side and top view of the experiment set up 36

2.29 Suction fan effect on vortex at α = 25° 36

2.30 Suction fan speed effects on vortex system at α = 25° 37

2.31 Delta wing model with nozzles near the apex 38

2.32 Vortex core location on blowing 39

2.33 Oil flow pattern above MAV for three configurations 40

2.34 Lift, drag and pitching moment coefficient of MAV 41

2.35 Delta winged UAV with middle propeller 43

2.36 Lift generated by MAV in motor ON and OFF modes 43

2.37 Leading edge extension configurations 44

2.38 Aerodynamic characteristics for leading extension

configurations with the motor ON and OFF modes

45

2.39 MAV aerodynamic characteristics 45

2.40 Flow visualization on MAV with propeller effects 46

2.41 Experimental setup and installation 47

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xiii

2.42 Lift and pitching moment coefficient on 65° swept delta

wing

48

2.43 Effects of pusher propeller actuation on 65° swept delta

wing upper surface pressure distribution

48

3.1 Framework of research 53

3.2 Existing delta-winged model with several propeller

locations

54

3.3 UAV wind tunnel model in CAD drawing 55

3.4 Dimensions of the UAV model 56

3.5 Pressure taps location on UAV model 57

3.6 Pressure taps numbering 58

3.7 UAV model configurations 59

3.8 Support system for the UAV model 60

3.9 Model installation for each configuration in wind tunnel 62

3.9 (c)-(d) 63

3.10 Electrical motor system of the UAV model 65

3.11 Propeller used for the UAV model 66

3.12 General process in data collection and data analysis 67

3.13 UTM-LST external balance 68

3.14 FKPS 30DP electronic pressure scanner 69

3.15 The notation of forces and moment 71

3.16 Flow chart of data correction 74

3.17 Solid blockage constant 77

3.18 CDu against CLu2 plot 78

3.19 Data Presentation 81

4.1 Measurement of CL and CD for clean wing 83

4.2 Effects of Reynolds number for clean configuration 85

4.2 (c) 86

4.3 Lift coefficient with angle of attack from experiment and

various sources

87

4.4 Effects of advance ratio on balance data (Front propeller) 88

4.4 (c) 89

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xiv

4.5 Effects of advance ratio on balance data (Middle

propeller)

89

4.5 (b)-(c) 90

4.6 Effects of advance ratio on balance data (Rear propeller) 91

4.6 (c) 92

4.7 Effects of propeller locations on lift coefficient 94

4.8 Effects of propeller locations on drag coefficient 95

4.9 Effects of propeller locations on pitching moment

coefficient

96

4.10 Effects of propeller locations on lift-drag ratio 97

4.11 Effects of Reynolds number on pressure distribution

above the wing

99

4.12 Propeller advance ratio effects on pressure distribution 100

4.12 (b)-(c) 101

4.13 The effects of front propeller on vortex properties 103

4.13 (c)-(d) 104

4.14 The effects of middle propeller on vortex properties 106

4.14 (c)-(d) 107

4.15 The effects of rear propeller on vortex properties 109

4.15 (c)-(d) 110

4.16 Surface pressure contour for clean wing at α=8° 112

4.17 Surface pressure contour for front propeller at α=8° 113

4.18 Surface pressure contour for middle propeller at α=8° 113

4.19 Surface pressure contour for rear propeller at α=8° 114

4.20 Surface pressure contour for clean wing at α=12° 115

4.21 Surface pressure contour for front propeller at α=12° 115

4.22 Surface pressure contour for middle propeller at α=12° 116

4.23 Surface pressure contour for middle propeller at α=12° 116

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xv

LIST OF SYMBOLS

c - Mean aerodynamic chord

C - Wind tunnel cross sectional area

CD - Drag force coefficient

CL - Lift force coefficient

CM - Pitching moment coefficient

CP - Pressure coefficient

D - Propeller diameter

f - Propeller frequency

F - Force

J - Propeller advance ratio

L - Spanwise length

L/D - Lift to drag ratio

M - Moment

P - Pressure

q - Dynamic pressure

Re - Reynolds number

S - Surface area

T - Temperature

v - Velocity

V - Volume

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xvi

Y/Cr - Chordwise location

Λ - Wing sweep angle

α - Angle of attack

β - Prandtl-Glauert compressibility factor

ε - Blockage component

µ - Dynamic viscosity

ζ - Angle between wing surface with vortex core

ρ - Air density

τ - Solid-blockage constant

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xvii

LIST OF APPENDICES

APPENDIX TITLE PAGE

A Delta-Winged UAV Model Drawing 129

B Kriging Method 146

C Polhamus Method 148

D Published Research Article 153

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CHAPTER 1

INTRODUCTION

1.1 Background of the Study

Unmanned Aerial Vehicle (UAV) is an aerial vehicle that operates without a

pilot on board. UAVs can be operated by the pilot at the ground control station

(controlled aircraft) or autonomous flying by preprogramed flight routes (autopilot

system). There are numerous types of UAVs available with various shapes and sizes.

UAVs exist in many types with different capabilities for the user requirements (Bento,

2008). Development of UAV was instigated by the piloted aircrafts evaluations (Koma

et al., 2008). The primary advantage of the UAV over piloted aircraft is portability.

UAV is easily to be stored, transported and launched in time-sensitive manner. Thus,

this made the operational cost of UAVs are cheaper compared to conventional aircraft.

UAVs can overcome the limitations of piloted aircraft such that unnecessary risk

exposure towards pilots and air crews during rescue missions or surveillance

operations. As UAVs are operated remotely, rescue and surveillance activities in

dangerous and non-accessible area can be performed without risking more lives

(Tajima et al., 2013; Nakashima et al., 2014). Aircraft with smaller design is becoming

essential to be used for limited period missions for both military and civil purposes

(Koma et al., 2008). Development of battery, wireless and Micro-Electromechanical

Systems (MEMS) have enable UAVs with increased capability at lower cost and

smaller in size (Hall et al., 2009). The current smallest UAV is Robo-fly shown in

Figure 1.1 is having insect imitation (entomopters) only weighing 106mg and capable

of search and rescue missions (Griffiths, 2014). UAVs becoming more favourable as

its special capability to operate lower than crewed aircraft. Furthermore, UAVs are

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capable to achieve a higher elevation than any land vehicles. The usage of UAVs can

be seen in 1940 when 15,000 units of radio controlled target drones were sold to United

States military for anti-aircraft training for World War II by Reginald Danny (Dillow,

2014). Currently, large and small companies are developing and designing UAVs

(Shafer & Green, 2010). Large companies conducting research on the UAVs design

by using computational fluid dynamics (CFD) and wind tunnel testing, enabling them

to have better potential design before flight testing.

Figure 1.1: Robo-fly UAV (Griffiths, 2014)

Numerous different groups have suggested reference standards for UAVs. One

of them is the European Association of Unmanned Vehicle Systems (EUROVS). The

EUROVS had classified UAVs based on several parameters such flight endurance,

altitude and size (Bento, 2008). Table 1.1 shows the classification of UAVs created

by EUROVS.

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Table 1.1: Classification of UAVs by EUROVS (Bento, 2008)

Category

(acronym)

Maximu

m Take

Off

Weight

(kg)

Maximu

m Flight

Altitude

(m)

Endura

nce

(hours)

Data Link

Range

(km)

Micro/

Mini

UAVs

Micro (MAV) 0.10 250 1 <10

Mini <30 150-300 <2 <10

Tactical

UAVs

Close Range

(CR)

150 3,000 2-4 10-30

Short Range

(SR)

200 3,000 3-6 30-70

Medium Range

(MR)

150-500 3,000-

5,000

6-10 70-200

Long Range

(LR)

- 5,000 6-13 200-500

Endurance

(ER)

500-1,500 5,000-

8,000

12-24 >500

Medium

Altitude, Long

Endurance

(MALE)

1,000-

1,500

5,000-

8,000

24-48 >500

Strategic

UAVs

High Altitude,

Long

Endurance

(HALE)

2,500-

12,500

15,000-

20,000

24-48 >2,000

Special

Task

UAVs

Lethal (LET) 250 3,000-

4,000

3-4 300

Decoys (DEC) 250 50-5,000 <4 0-500

Stratospheric

(Strato)

TBD 20,000-

30,000

>48 >2,000

Exo-

stratospheric

(EXO)

TBD >30,000 TBD TBD

In the past, UAVs had been used mostly for the military purposes. Currently,

UAVs is starting to be used in scientific, commercial and public safety tasks (Bento,

2008). UAVs purpose to carry out civil missions’ potential was discovered when

UAVNET (UAV Network) project is launched in October 2001. This is followed by

another two projects, USICO (UAV Safety Issues for Civil Operation) and CAPECON

(Civil UAV Applications and Economic Effectivity and Potential Configuration

Solutions) in May 2012 (Smith & Rajendran, 2014). Dillow (2014) stated the usage of

UAVs for non-military purposes have been escalating in developed countries such as

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Japan, France, United Kingdom and Australia. UAVs are a potential device to be used

in various applications such as in agriculture, map building, traffic surveillance,

construction, film production, search and rescue mission and weather forecasting. For

the meteorology field, UAV is used to observe development of storms (Handwerk,

2013). From the program, the valuable surveillance in stormy area can be captured by

the UAV which cannot be performed by the manned plane. In topography field,

Sensefly and Drone Adventures promotes usage of UAV for civil application by

mapping Matterhorn mountain, which is located on the border between Switzerland

and Italy (Carrol, 2013). For agriculture purposed, UAV cameras can be used to

monitor growth of plants at specific field section. Current UAV is equipped with

infrared camera enabling plant health observation based on the photosynthesis

efficiency (Handwerk, 2013). One of the flying UAV used for civil application is

LA100 which is shown in Figure 1.2. LA100 is produced by Lehmann Aviation Ltd

and having 92 cm wingspan and 1.25 kg in weight. LA100 is designed for civil

applications such as reconnaissance, security, mapping, survey and monitoring. The

UAVs are able to take still aerial images and real-time videos.

Figure 1.2: LA100 UAV (Lehmann Aviation, 2014)

92 cm

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1.2 Delta-Winged UAV

The advancement of the technology has triggered essential of aircraft that

capable of higher speed and manoeuvre. Delta wing configurations are suitable for

both supersonic and subsonic aircraft (Pevitt & Alam, 2014). The delta wing design

initially was carried out in Germany in the early 1940s (Whitford, 1987). After the

Allied won the Second World War, delta wing design was appeared on drawing for

major aircraft design. The delta wing is having triangle appearance on wing plan and

is named after Greek letter delta (Δ) as their similar shape (Teli et al., 2014). The delta

wing configuration can be divided into slender and non-slender wing based on their

swept angle (Λ). Slender wing having very high swept angle which are Λ>60°. Delta

wing is categorised in fixed-wing UAVs alongside with flying wing class and blended

winged body (BWB) class. There is different type of delta wings, which are standard

delta, tailed delta, cropped delta, compound delta, cranked arrow, ogival delta, lambda

delta and diamond wing. The delta wing configurations are shown in Figure 1.3.

(a) Standard

delta

(b) Tailed Delta (c) Cropped delta

(d) Compound

delta

(e) Cranked

arrow

(f) Ogival delta (e) Lambda

(f) Diamond

Figure 1.3: Delta wing configurations (Pevitt & Alam, 2014)

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Currently, delta wing design is implanted in UAVs application (Tricoche et al.,

2004). Delta planform is favourable in the UAVs design because of the excellent

properties at a higher angle of attack (Polhamus, 1966). Delta wing configuration in

UAV shows aerodynamic advantages over conventional design in power efficiency

and lower ratio of wetted area to volume (Tajima et al., 2013). Delta-winged UAV

design is always simple and robust. Thus, the delta wing aircraft is having less complex

design and having high durable design accompanied by extra internal volume for

power source and aircraft system. Normally, delta wing UAV is stronger than a similar

swept wing UAV. The delta winged UAV can be built stronger than swept wing

aircraft as the spar attaches with the fuselage afar in front of the centre of gravity. Since

delta wing aircraft having simple design, it is likely to have less impact during crash

and could minimise the possible damage that may occur. The manufacturing cost of

the delta wing could be reduced as it need less materials. Figure 1.4 shows several

existing flying delta wing UAVs.

Figure 1.4: Several examples of delta winged UAVs (RCGroups.com, 2014;

SkyHighHobby.com, n.d.)

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1.3 Research Objective

The aim of this project is to investigate the effects of propeller locations on the

aerodynamic and vortex characteristics above sharp-edged delta wing UAV. In order

to achieve the said objectives, the research will;

(i) Measure the aerodynamic characteristics of delta-winged UAV with and

without rotating propeller.

(ii) Investigate the effects of propeller locations on the vortex characteristics

of the delta-winged UAV model.

(iii) Investigate the effects of advance ratio for all propeller configurations on

the delta-winged UAV.

1.5 Scope of the Research

As the main objective of this project is to investigate the effects of propeller

locations on the vortex properties above non-slender sharped-edge delta wing, the

scopes of this research are divided into four stages:

(i) Literature review on delta wing UAV and delta wing flow topology.

(ii) Model design and fabrication of the UAV model in standard delta category.

(iii) Wind tunnel experiment of the model without the propeller, called as clean

wing configuration.

(iv) Wind tunnel experiment of the model with several propeller locations. In

this project, the locations of the propeller were set at three stations:

In front of the wing.

In the middle part of the wing.

In the rear part of the wing.

It has been decided that the motor speed was set at 6,000 rpm since most of the UAVs

are flying at this speed.

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1.6 Significance of the Research

This research would provide a better insight into the aerodynamic

characteristic and the vortex properties above delta-winged UAV under the effects of

rotating propeller installed on the wing at three locations, i.e. front, middle and rear.

The speed of the motor was set at 6,000 rpm based on the standard range of propeller

speed in the same category of UAV. Two measurements techniques which are steady

balance data and surface pressure measurement are used to evaluate the UAV

performance.

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