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iii
THE DEVELOPMENT OF A FIXED WING AIRCRAFT ANALYSIS AND
DESIGN FLIGHT DYNAMIC SOFTWARE
AHMAD ESHTIWEY AHMAD ALAIAN
A thesis submitted in 18 / 02 / 2016
fulfillment of the requirement for the award of the
Doctor of Philosophy in Mechanical and Manufacturing Engineering
Faculty of Mechanical and Manufacturing Engineering
Universiti Tun Hussien Onn Malaysia
JANUARY 2016
v
ACKNOWLEDGEMENT
This research thesis was made possible through the enormous help and great support
from everyone, including: my father, mother, wife, teachers and family. I would like
to dedicate my acknowledgment of gratitude toward the following significant
advisors and contributors:
First and foremost, I would like to thank Ir. Dr. Bambang Basuno for his endless
support and encouragement. He kindly read my paper and offered invaluable detailed
advices on grammar, organization, and the theme of the thesis.
Second, I would like to thank Assoc Prof. Dr. Zamri Bin Omar who read my thesis
and he provided me with valuable feedbacks and advice. In addition I would like to
thank all the other professors who have taught me about Mechanical Engineering and
Manufacturing in general and Aeronautics department in particular and helped me to
gain my doctoral degree.
Finally, I would like to sincerely thank my parents, wife, daughters, brothers, sisters,
friends, and colleagues who provided me with enormous support throughout my
journey. The product of this research work would not be possible without all of them.
vi
ABSTRACT
The present work focused on the development of computer software for flight
dynamic analysis and controlling the behavior of a fixed-wing aircraft. For a given
aircraft geometry, mass and inertia properties, and flight conditions, the software was
designed in such a way to start the estimation of aerodynamic characteristics,
trimmed flight, stability analysis through linearized approach as well as non-
linearized, and finally the control design of the flying behavior by using PID
controller method. The estimation of aerodynamic characteristics used the semi-
empirical aerodynamic method as used by Roskam. The trimmed flight conditions
were solved through trimmed flight equations iteratively. The linearized form of
flight dynamic equations in longitudinal as well as in lateral direction were solved
using the transfer function approach and state-space method. Whilst, non-linear flight
dynamic equations were solved using the Simulink. Three different PID controller
designs were developed to control the aircraft to follow a particular flight behavior.
The developed computer code was written in MATLAB programming language and
grouped into several modules. The validation results were carried out by comparing
the results of each module to other results available in the literature. The developed
computer code was applied to the case of five aircraft. They were named Cessna 182,
Cessna 310, Piper Cherokee PA 28-162, Learjet 24, and Cessna 620. The first three
aircraft were propeller piston engine aircraft. The fourth aircraft was a jet engine
aircraft while the fifth aircraft represented a turboprop aircraft. The flight dynamics
behavior motion which consisted of 22 flight variables were obtained by solving the
governing equation of flight after the aerodynamic characteristics data were
established and the trimmed fight conditions were solved. A particular flight variable
can be set up to have a particular behavior that follows the movement of the control
surface operations. Various control surface movements were simulated to ensure the
vii
designed PID controller was really providing a particular flight behavior. Through
the implementation of five types of aircraft models, the developed computer code
represents a useful tool for flight dynamic analysis and control design for a fixed-
wing aircraft.
viii
ABSTRAK
Kajian ini memfokuskan pembangunan perisian komputer untuk menganalisis
dinamik penerbangan dan kawalan tingkah laku pesawat bersayap tetap. Perisian
bagi sesuatu pesawat direka berdasarkan geometri, sifat seperti jisim dan inersia, dan
keadaan penerbangan. Perisian tersebut digunakan untuk membuat anggaran awal
bagi ciri-ciri aerodinamik, potongan sayap pesawat, analisis kestabilan melalui
pendekatan linear dan juga tak linear, disusuli dengan kawalan reka bentuk perilaku
penerbangan dengan menggunakan kaedah pengawal PID. Penganggaran ciri
aerodinamik dibuat dengan menggunakan kaedah aerodinamik separa empirikal
sebagaimana yang diguna pakai oleh Roskam. Keadaan potongan sayap pesawat
diselesaikan melalui persamaan potongan sayap pesawat secara lelaran. Persamaan
dinamik penerbangan berbentuk linear dalam arah membujur dan juga sisi
diselesaikan dengan menggunakan pendekatan fungsi pemindahan dan kaedah ruang
keadaan. Seterusnya, persamaan dinamik penerbangan tak linear diselesaikan dengan
menggunakan Simulink. Tiga buah reka bentuk pengawal PID yang berbeza
dibangunkan untuk mengawal pesawat supaya mengikut tingkah laku penerbangan
tertentu. Kod komputer yang dibangunkan ditulis dalam bahasa pengaturcaraan
MATLAB dan dikumpulkan dalam beberapa modul. Keputusan pengesahan
dijalankan dengan membandingkan keputusan setiap modul dengan keputusan yang
terdapat dalam kajian terdahulu. Kod komputer yang dibangunkan kemudiannya
diaplikasikan pada lima kes pesawat. Model pesawat tersebut dikenali sebagai
Cessna 182, Cessna 310, Piper Cherokee PA 28-162 , Learjet 24 dan Cessna 620.
Tiga pesawat pertama yang disenaraikan merupakan pesawat berenjin omboh
bebaling. Pesawat keempat merupakan pesawat berenjin jet, manakala pesawat
kelima mewakili pesawat berenjin turboprop. Tingkah laku gerakan dinamik
penerbangan yang terdiri daripada 22 pemboleh ubah penerbangan diperoleh dengan
ix
menyelesaikan persamaan penentu penerbangan setelah data berkenaan ciri
aerodinamik dibangunkan dan keadaan potongan sayap pesawat diselesaikan.
Pemboleh ubah penerbangan tertentu boleh ditetapkan dengan tingkah laku tertentu
mengikut pergerakan operasi permukaan kawalan. Pelbagai pergerakan permukaan
kawalan disimulasikan untuk memastikan pengawal PID yang direka benar-benar
menepati tingkah laku penerbangan tertentu. Melalui pelaksanaan lima jenis model
pesawat, kod komputer yang dibangunkan menjadi alat yang berguna untuk
menganalisis dinamik penerbangan dan reka bentuk kawalan bagi pesawat bersayap
tetap.
x
CONTENTS
TITLE iii
ACKNOWLEDGEMENTS v
ABSTRACT vi
CONTENTS x
LIST OF FIGURES xiv
LIST OF TABLES xxii
LIST OF SYMBOLS xxv
LIST OF APPENDIXES xxvii
CHAPTER 1 INTRODUCTION 1
1.1 Background of study 1
1.2 Problem statement 4
1.3 Objectives 5
1.4 Scope of work 6
1.5 Research methodology 9
1.6 The results of the research work 9
1.7 Organization of the thesis 10
CHAPTER 2 LITERATURE REVIEW 12
2.1 Aircraft flight dynamics 12
2.2 The governing equation of flight motions 15
2.3 Simplified forms of the governing equation of
flight motion 25
2.3.1 Simplified longitudinal direction
form of equations 26
2.3.2 Simplified lateral-direction form of
xi
equations 29
2.4 The trim condition governing equation 30
2.5 Flying and handing qualities 33
2.5.1 Longitudinal flying qualities 34
2.5.1.1 Static response 34
2.5.1.2 Phugoid response 34
2.5.1.3 Short period response 34
2.5.2 Lateral flying qualities 35
2.5.2.1 Rolling motion 35
2.5.2.2 Spiral stability 36
2.5.2.3 Lateral directional oscillations-Dutch
roll
37
2.6 Compression between linear and non-linear
equation
37
2.7 An overview of the solution of the
governing equation for flight motion
38
2.7.1 Euler’s method 40
2.7.2 The second order Runge-Kutta method 41
2.7.3 The fourth order Runge-Kutta method 41
2.7.4 Adams-Bashforth method of order
three
41
2.8 An overview on the manner of controlling
the aircraft movement
42
2.9 Aircraft controller design 44
2.10 The flight dynamics software 46
2.11 The flight dynamics software development in
the past
48
CHAPTER 3 METHODOLOGY 51
3.1 Introduction 51
3.2 The aerodynamics characteristics estimation 52
3.3 The aircraft dimensional stability and control
derivatives
57
3.4 The method of solving the equation of flight
xii
motion 59
3.4.1 The solution of flight motion based on
state-space approach
59
3.4.2 The solution of flight motion based on
transfer functions approach
62
3.5 The classical PID control design estimation 70
3.5.1 The basic idea of the control system
design
72
3.5.2 The technique in developing PID
controller
76
3.6 Non-linear simulation aircraft behaviour 80
CHAPTER 4 RESULTS AND DISCUSSION 82
4.1 Introduction 82
4.2 Longitudinal and lateral directional dynamic
stability behaviours
82
4.2.1 Input data 85
4.2.2 The output and the results of the
longitudinal and lateral directional
dynamic stability behaviours
88
4.2.2.1 The stability derivatives of longitudinal
and lateral directions
88
4.2.2.2 The solution for flight motion 89
4.2.3 Time history and stability behavior of
aircrafts
97
4.2.3.1 Time history or stability behavior in the
longitudinal direction
100
4.2.3.2 Time history and stability behavior in
the lateral direction
111
4.3 Controller design 138
4.3.1 The results of Cessna 182 controller
design
140
4.3.1.1 The longitudinal direction controller
design
140
xiii
4.3.1.2 The lateral direction controller design 142
4.3.2 Time history of Cessna 182 aircraft 152
4.3.2.1 Time history of pitch angle controller 153
4.3.2.2 Time history of roll angle controller 158
4.3.2.3 Time history of yaw angle controller 168
4.4 The non-linear simulation aircraft behaviour 182
4.4.1 The geometry and the overall
performance data of Piper Cherokee PA
28-161 Warrior
182
4.4.2 The evaluation of the aerodynamics
characteristics of the Piper Cherokee
PA 28-161
188
4.4.3 The Simulink diagram for the Piper
Cherokee PA 28-161
191
4.4.4 The estimation of flight dynamics
behavior with Simulink
194
4.4.5 Comparison between non-linear and
linear models
209
4.5 Summary 214
CHAPTER 5 CONCLUSION AND FUTURE WORK 217
5.1 Introduction 217
5.2 Conclusion 217
5.3 Contribution and the novelty of research 218
5.4 Future work 219
REFERENCES 221
APPENDIX 231
xiv
LIST OF FIGURES
1.1 The automatic and the manual flight control loops 3
1.2 Flight dynamics analysis and design procedure 7
2.1 The locations of the origin of the coordinate systems 16
2.2 The orientation of body axis, stability axis, and wind
axis
18
2.3 Body axis coordinate system 18
2.4a Definitions of aerodynamic forces, thrust, and
acceleration gravitation in body axis coordinate
19
2.4b Definitions of moments, linear, and angular velocity
in body axis coordinate system
19
2.5 Flowchart for non-linear simulation steps 40
2.6 The conventional aircraft 43
2.7 Unity feedback system 45
3.1 A simplified body diagram of the mass, spring and
damper
73
3.2 The block diagram of the vehicle as an open loop
system
73
3.3 The displacement response of mass, spring and
damper as an open loop system due to a unit step
function
74
3.4 The control system with a unity feedback 75
3.5 The displacement response of mass, spring and
damper as a closed-loop system due to a unit step
function
75
3.6 A closed loop system of the dynamic vehicle’s
xv
equation and PID controller 77
3.7 The step response of Method I controller approach 78
3.8 The step response of Method II controller approach 79
3.9 The step response of PID SISO controller approach 79
4.1 Two types of propeller driven aircrafts 84
4.2 Two types of turbo driven aircrafts 84
4.3 MATLAB start menu for the direction analysis 84
4.4 MATLAB start menu for the aircraft model analysis 85
4.5a MATLAB start menu for longitudinal direction 99
4.5b MATLAB start menu to select the lateral effect
control surfaces
99
4.6a Longitudinal direction responses following elevator
single doublet impulse maneuvers of Cessna 182
100
4.6b Longitudinal direction responses following elevator
single doublet impulse maneuvers of Cessna 310
101
4.6c Longitudinal direction responses following elevator
single doublet impulse maneuvers of Learjet 24
101
4.6d Longitudinal direction responses following elevator
single doublet impulse maneuvers of Cessna 620
102
4.7a Longitudinal direction responses following elevator
multiple doublets impulse maneuvers of Cessna 182
103
4.7b Longitudinal direction responses following elevator
multiple doublets impulse maneuvers of Cessna 310
104
4.7c Longitudinal direction responses following elevator
multiple doublets impulse maneuvers of Learjet 24
105
4.7d Longitudinal direction responses following elevator
multiple doublets impulse maneuvers of Cessna 620
105
4.8a Longitudinal direction responses following elevator
single doublet maneuvers of Cessna 182
106
4.8b Longitudinal direction responses following elevator
single doublet maneuvers of Cessna 310
106
4.8c Longitudinal direction responses following elevator
single doublet maneuvers of Learjet 24
107
xvi
4.8d Longitudinal direction responses following elevator
single doublet maneuvers of Cessna 620
107
4.9a Longitudinal direction responses following elevator
multiple doublets maneuvers of Cessna 182
108
4.9b Longitudinal direction responses following elevator
multiple doublets maneuvers of Cessna 310
108
4.9c Longitudinal direction responses following elevator
multiple doublets maneuvers of Learjet 24
109
4.9d Longitudinal direction responses following elevator
multiple doublets maneuvers of Cessna 620
109
4.10a Lateral direction responses following aileron single
duplet impulse maneuvers of Cessna 182
112
4.10b Lateral direction responses following aileron single
duplet impulse maneuvers of Cessna 310
112
4.10c Lateral direction responses following aileron single
duplet impulse maneuvers of Learjet 24
113
4.10d Lateral direction responses following aileron single
duplet impulse maneuvers of Cessna 620
113
4.11a Figure 4.11a: Lateral direction responses following
aileron multiple doublets impulse maneuvers of
Cessna 180
115
4.11b Lateral direction responses following aileron multiple
doublets impulse maneuvers of Cessna 310
115
4.11c Lateral direction responses following aileron multiple
doublets impulse maneuvers of Learjet 24
116
4.11d Lateral direction responses following aileron multiple
doublets impulse maneuvers of Cessna 620
116
4.12a Lateral direction responses following aileron single
doublet maneuvers of Cessna 182
117
4.12b Lateral direction responses following aileron single
doublet maneuvers of Cessna 310
117
4.12c Lateral direction responses following aileron single
doublet maneuvers of Learjet 24
118
xvii
4.12d Lateral direction responses following aileron single
doublet maneuvers of Cessna 620
118
4.13a Lateral direction responses following aileron multiple
doublets maneuvers of Cessna 182
119
4.13b Lateral direction responses following aileron multiple
doublets maneuvers of Cessna 310
119
4.13c Lateral direction responses following aileron multiple
doublets maneuvers of Learjet 24
120
4.13d Lateral direction responses following aileron multiple
doublets maneuvers of Cessna 620
120
4.14a Lateral stability behavior of Cessna 182 following
rudder single duplet impulse maneuvers
123
4.14b Lateral stability behavior of Cessna 310 following
rudder single duplet impulse maneuvers
123
4.14c Lateral stability behavior of Learjet 24 following
rudder single duplet impulse maneuvers
124
4.14d Lateral stability behavior of Cessna 620 following
rudder single duplet impulse maneuvers
124
4.15a Lateral stability behavior of Cessna 182 following
rudder multiple doublets impulse maneuvers
125
4.15b Lateral stability behavior of Cessna 310 following
rudder multiple doublets impulse maneuvers
125
4.15c Lateral stability behavior of Learjet 24 following
rudder multiple doublets impulse maneuvers
126
4.15d Lateral stability behavior of Cessna 620 following
rudder multiple doublets impulse maneuvers
126
4.16a Lateral stability behavior of Cessna 182 following
rudder single doublet maneuvers
127
4.16b Lateral stability behavior of Cessna 310 following
rudder single doublet maneuvers
127
4.16c Lateral stability behavior of Learjet 24 following
rudder single doublet maneuvers
128
4.16d Lateral stability behavior of Cessna 620 following
xviii
rudder single doublet maneuvers 128
4.17a Lateral stability behavior of Cessna 182 following
rudder multiple doublets maneuvers
129
4.17b Lateral stability behavior of Cessna 310 following
rudder multiple doublets maneuvers
129
4.17c Lateral stability behavior of Learjet 24 following
rudder multiple doublets maneuvers
130
4.17d Lateral stability behavior of Cessna 620 aircraft
following rudder multiple doublets maneuvers
130
4.18 The aircraft elevator deflection as pulse 132
4.19a Aircraft velocity stability behavior of four aircraft
models following the elevator deflection
133
4.19b Angle of attack stability behavior of four aircraft
models following the elevator deflection
133
4.19c Pitch angle stability behavior of four aircraft models
following the elevator deflection
134
4.20a Side slip angle stability behavior of four aircraft
models following the aileron deflection
135
4.20b Roll angle stability behavior of four aircraft models
following the aileron deflection
135
4.20c Yaw angle stability behavior of four aircraft models
following the aileron deflection
136
4.21a Side slip angle stability behavior of four aircraft
models following the rudder deflection
136
4.21b Roll angle stability behavior of four aircraft models
following the rudder deflection
137
4.21c Yaw angle stability behavior of four aircraft models
following the rudder deflection
137
4.22 The elevator step response from method I and method
II controller approach
141
4.23 The elevator step response from SISO controller
approach
141
4.24 The aileron step response from method I control
xix
design approach 143
4. 25 The aileron step response with method II control
design approach
144
4. 26 The aileron step response from SISO control design
approach
144
4. 27 The rudder step response from method I control
design approach
146
4. 28 The rudder step response from method II control
design approach
146
4. 29 The rudder step response from SISO control design
approach
146
4.30 The aileron step response from method I control
design approach
148
4. 31 The aileron step response from method II control
design approach
148
4. 32 The aileron step response from SISO control design
approach
149
4. 33 The rudder step response from method I control
design approach
150
4. 34 The rudder step response from method II control
design approach
151
4. 35 The rudder step response from SISO control design
approach
151
4. 36 The various manners of the elevator defection 153
4. 37 Pitch angle behaviors due to the elevator of single
doublet impulse
154
4. 38 Pitch angle controller behavior due to multiple
doublet impulses
155
4. 39 Pitch angle controller behavior due to elevator single
doublet
157
4. 40 Pitch angle controller behavior due to elevator
multiple doublets
158
4.41 The aileron control surfaces deflection 159
xx
4.42 The rudder control surfaces deflection 159
4.43 The stability behavior for Cessna 182 before and after
applying the control design approach (Aileron)
160
4.44 The stability behavior for Cessna 182 before and after
applying the control design approach (Rudder)
161
4.45 The stability behavior for Cessna 182 before and after
applying the control design approach (Aileron)
162
4.46 The stability behavior for Cessna 182 before and after
applying the control design approach (Rudder)
163
4.47 The stability behavior for Cessna 182 before and after
applying the control design approach (Aileron)
164
4.48 The stability behavior for Cessna 182 before and after
applying the control design approach (Rudder)
165
4.49 The stability behavior for Cessna 182 before and after
applying the control design approach (Aileron)
166
4.50 The stability behavior for Cessna 182 before and after
applying the control design approach (Rudder)
167
4.51 The stability behavior for Cessna 182 before and after
applying the control design approach (Aileron)
169
4.52 The stability behavior for Cessna 182 before and after
applying the control design approach (Rudder)
170
4.53 The stability behavior for Cessna 182 before and after
applying the control design approach (Aileron)
171
4.54 The stability behavior for Cessna 182 before and after
applying the control design approach (Rudder)
172
4.55 The stability behavior for Cessna 182 before and after
applying the control design approach (Aileron)
173
4.56 The stability behavior for Cessna 182 before and after
applying the control design approach (Rudder)
174
4.57 The stability behavior for Cessna 182 before and after
applying the control design approach (Aileron)
175
4.58 The stability behavior for Cessna 182 before and after
applying the control design approach (Rudder)
176
xxi
4.59 The elevator control surface setting at -2.0 degree 177
4.60 The roll angle response with aileron set at -2.0o 178
4.61 The roll angle response with rudder set at -2.0o 179
4.62 The yaw angle response with aileron set at -2.0o 180
4.63 The yaw angle response with rudder set at -2.0o 181
4.64 Three side views drawing of Piper Cherokee PA 28-
161 aircraft
183
4.65 Aircraft simulation with steady state winds 191
4.66 The velocity in x-direction u as function of time at a
trimmed flight condition.
197
4.67 The angle of attack as function of time at a trimmed
flight condition.
197
4.68 The velocity in x-direction (u) as function of time 198
4.69 The velocity in y-direction (v) as function of time 200
4.70 The velocity in z-direction (w) as function of time 201
4.71 The pitch angle θ as function of time 202
4.72 The yaw angle ψ as function of time 203
4.73 The roll angle ϕ as function of time 204
4.74 Angle of attack α as function of time 205
4.75 Side slip angle β as function of time 207
4.76 Flight bath angle γ as function of time 208
4.77 The angle of attack α comparison 209
4.78 The sideslip angle β comparison 210
4.79 Pitch angle comparison 211
4.80 The yaw angle ψ comparison 212
4.81 The roll angle ϕ comparison 213
xxii
LIST OF TABLES
2.1 The definitions of notations in describing forces,
moment, and velocity components
20
2.2 Phugoid mode flying qualities 34
2.3 Short period mode damping ratio specification 35
2.4 Short period mode damping ratio specification 35
2.5 Bank angle specification 36
2.6 Spiral mode stability specification 37
2.7 Dutch roll mode specification 37
3.1 The required aerodynamics characteristics in solving
flight dynamic equation
53
3.2 The Geometry and the basic aerodynamic data needed
in estimation of the aircraft aerodynamic
characteristics
54
3.3 Longitudinal dimensional stability and control
derivatives
58
3.4 Lateral dimensional stability and control derivatives 58
3.5 The values of the gains 79
4.1 Aircraft geometric data 85
4.2 Aircraft flight condition data 86
4.3 Aircraft mass and inertia data 86
4.4 Aircraft longitudinal steady state input data 86
4.5 Aircraft stability derivative data 86
4.6 Aircraft control derivatives data 86
4.7 The longitudinal direction stability derivative
calculations
88
xxiii
4.8 The lateral direction stability derivatives calculations 89
4.9 Setting up matrix A for longitudinal direction 90
4.10 Setting up matrix B for longitudinal direction 90
4.11 Setting up matrix C for longitudinal direction 91
4.12 Setting up matrix A for lateral direction 92
4.13 Setting up matrix B for lateral direction 92
4.14 Setting up matrix E for lateral direction 94
4.15 Longitudinal direction transfer function in terms of u 95
4.16 Longitudinal direction transfer function in terms of α 95
4.17 The longitudinal transfer function in terms of 96
4.18 Lateral direction transfer function in terms of β 96
4.19 Lateral direction transfer function in terms of ϕ 96
4.20 Lateral direction transfer function in terms of ψ 97
4.21 The maximum and minimum values of α, U, and θ
related to the elevator maneuvers
110
4.22 The expected time to reach the steady state behavior
related to the elevator maneuvers (Sec)
110
4.23 The maximum and minimum values of β, ϕ, and ψ
with aileron maneuver
121
4.24 The expected time to reach the steady state behavior
related to the aileron maneuvers (Sec)
121
4.25 The maximum and minimum values of changes in β,
ϕ, and ψ with rudder maneuver
131
4.26 The expected time to reach the steady state behavior
related to the rudder maneuvers (Sec)
131
4.27 Gains value of the controller design approaches 142
4.28 Pitch angle controller transfer functions 142
4.29 The values of the gain 145
4.30 Roll angle controller transfer function due to the
aileron maneuvers
145
4.31 The values of the gain 147
4.32 Roll angle controller transfer function due to the
rudder maneuvers
147
xxiv
4.33 The values of the gain 149
4.34 Yaw angle controller transfer function due to the
aileron maneuvers
150
4.35 The values of the gain 152
4.36 Yaw angle controller transfer function due to the
rudder maneuvers
152
4.37 The geometry and the aerodynamic data of Piper
Cherokee PA 28-161 Warrior aircraft
183
4.38 The aircraft geometry and the aerodynamic data 185
4.39 The mass and the moment of inertia Piper Cherokee
28-161 aircraft
189
4.40 The aircraft solution at trim condition 189
4.41 The solution of the aircraft aerodynamics characters 189
4.42 MATLAB flight parameter outputs 192
4.43 The variable state parameters 193
4.44 The scenarios of control surfaces and the engine thrust
during the aircraft in flight
194
4.45 The control surfaces and the engine thrust setting at
trim condition
195
4.46 The behavior of the flight parameters 195
4.47 Responses of the three controller design approaches 215
xxv
LIST OF SYMBOLS
U - X-direction trim velocity
V - Y-direction trim velocity
W - Z-direction trim velocity
u - Velocity in X-direction
v - Velocity in Y-direction
- Total velocity
w - Velocity in Z-direction
- Pitch angle
Ψ - Yaw angle
ϕ - Roll angle
α - Angle of attack
β - Side slip angle
γ - Flight path angle.
p - Roll rate
q - Pitch rate
r - Yaw rate
L - Rolling moment
M - Pitching moment
N - Yawing moment
Ixx - Moment of inertia about X-axis
Iyy - Moment of inertia about Y-axis
Izz - Moment of inertia about Z-axis
T - Thrust
Cx - The aircraft axial force coefficient
CY - The aircraft side force coefficient
xxvi
Cz - The aircraft normal force coefficient
C - The aircraft rolling moment coefficient
Cm - The aircraft pitching moment coefficient
Cn - The aircraft yawing moment coefficient
N - The engine rotational speed in radian
Ixe - The engine moment of inertia of the rotating mass
- The dynamic pressure is equal to
C.G - Aircraft’s center of gravity
S - The wing area reference
- Horizontal tail area
- Wing incidence angle
- The wing span.
- The air density
CL - Aircraft lift coefficient
CD - Aircraft drag coefficient
- Aircraft mass
CY - Aircraft side force coefficient
- Total velocity
- Elevator deflection angle
- Aileron deflection angle
- Rudder deflection angle
- Aircraft engine thrust
- Time
CA - Axial force coefficient
CN - Normal force coefficient
- Wing twist angle
- Distance in X-direction
- Distance in y-direction
- Flight altitude
- Aircraft fuselage average width
M - Mach number
xxvii
LIST OF APPENDIXES
APPENDIX TITLE PAGE
A The aerodynamic characteristics estimation 231
B Examples of how the figures are being
implemented in the software
285
C List of publications during the research work 289
CHAPTER 1
INTRODUCTION
1.1 Background of study
The system that is used to control the aircraft when flying is called flight control
system (FCS) [1]. The flight control system (FCS) deflects the aircraft control
surface to control the aircraft. This system can be operated in different manners; the
first controls the aircraft, which can be done by human [2], while the second is
controlled by computer (AFCS), which is easier, faster and more efficient [3].
In the early days, in order to give the necessary control surface deflections to control
the aircraft, the flight control system (FCS) had been operated mechanical by using
cables and pulleys [4]. However, the new technologies have brought with them the
fly-by-wire [5]. In this system, electrical signals are sent to the control surfaces to
make the required control surface deflections. The signals are sent to the aircraft
control surface by using a computer (FC/FCC) [1].
Moreover, there are several advantages in applying the automatic flight control
system, such as: i) the computer has higher reaction velocity compared to the pilot,
ii) it is not subject to concentration loss and fatigue, and iii) the computer can more
accurately detect the state the aircraft is in (computers can handle huge amounts of
data better and also need not read any small indicator to identify, for example, the
2
velocity or the height of the aircraft). However, there is a downside to the (AFCS); it
is only designed for a certain flight envelope. It means, when the aircraft is outside
the flight envelope, the system cannot operate the aircraft anymore. Besides, the
Automatic flight control system can be categorized into four different types based
on the level of difficulty of the task [1].
(a) (AFCS) as the trimmed flight-holding system.
(b) (AFCS) as the stability augmentation system.
(c) (AFCS) as the command augmentation system.
(d) (AFCS) as the stability maker and command optimization.
The basic elements in the control information loop are the plant (the
controlled system) and the controller. For an aircraft, the controlled system
consists of control apparatus, control surface, and the aircraft. Meanwhile, the
controller part consists of three subsystems, namely: i) aircraft motion sensor, ii)
aircraft motion information processor and iii) control command generator. Figure 1.1
shows the functional diagram of the manual and the automatic control system
for an aircraft. The diagram shows that the primary interface between the
controlled and controller systems can be divided into two parts: i) front-end
interface, which is the aircraft sensory system and ii) back-end interface, which is
the control command generator [1] [6].
3
Figure 1.1: The automatic and the manual flight control loops [1]
Apart from that, the flight control system of an aircraft FCS generally consists of
three important parts. These three parts are: i) the stability augmentation system SAS
that augments the stability of the aircraft. This is done by using the control surfaces
to make the aircraft more stable. A good example of a part of the SAS is the phugoid
damper (similarly, the yaw damper). A phugoid damper uses the elevator to reduce
the effects of the phugoid: it damps it. The SAS is always on when the aircraft is
flying. Without it, the aircraft is less stable or possibly even unstable, ii) the control
augmentation system CAS is a helpful tool for the pilot to control the aircraft. For
example, the pilot can tell the CAS to keep the current heading. The CAS then
follows this command. With this, the pilot does not continually have to compensate
Controller motion Aircraft motion
HUMAN CONTROLLER
AUTOMATIC CONTROLLER
Command generator Information processor Motion sensor
Pilot’s hands, feet
voices Pilot’s brain Cockpit display,
window view, pilot’s
eyes and ears
Actuator FCC RLG, Aces, Pilot
Command generator Information processor Fluids dynamics/
inertial sensors
4
for heading changes himself, and iii) finally, the automatic control system takes
things one step further. It automatically controls the aircraft. It does this by
calculating (for example) the roll angles of the aircraft that are required to stay on a
given flight path. It then makes sure that these roll angles are achieved. In this way,
the airplane is controlled automatically.
There are important differences between the above three systems. First, the SAS is
always on, while the other two systems are only on when the pilot needs them.
Second, there is the matter of reversibility. In the CAS and the automatic control, the
pilot feels the actions that are performed by the computer. In other words, when the
computer decides to move a control panel, the stick / pedals of the pilot move along.
This makes these systems reversible. The SAS, on the other hand, is not reversible:
the pilot does not receive any feedback. The reason for this is simple. If the pilot
receives feedback [7], he would only feel the annoying vibrations. This is of course
undesirable. Therefore, in order to develop such flight control system, the knowledge
of flight dynamic behavior of the aircraft is required [8] [9]. This aircraft flight
dynamic behavior can be determined by solving the governing equation of flight
motion [10] [11]. The aerodynamics forces and the moment act as the input to the
governing equation of flight motion that enables the evaluation of the flight
dynamics behavior to be done at various control surfaces settings. Besides, with the
solution of flight dynamics equation, one can design an appropriate controller, if the
aircraft is decided to have a particular flight behavior.
1.2 Problem statement
The flight dynamics behavior of most aircrafts can be controlled through control
surfaces and engine thrust. With the presence of pilot in the cockpit, the movement
of the aircraft is completely under the control of the pilot. Besides, a pilot can operate
the control surface or adjust the engine thrust in order to keep the aircraft flying as
expected at any time. Nonetheless, unfortunately, the way an aircraft behaves
depends on the flight conditions. On top of that, the flight condition is strongly
influenced by its atmospheric environment. As a result, the work load of the pilot is
increased if the atmospherics environments always change. Hence, the aircraft flight
control system has been introduced to reduce the work load of the pilot in controlling
5
the aircraft movement. Basically, the behavior of the aircraft can be identified and
controlled if all flight variables related to the flight behavior are evaluated in respect
to time. Strictly speaking, 21 flight variables are available to describe the flight
behavior of an aircraft during flight [12]. These 21 flight variables are the three
components of velocity at trim (U, V, W), the three components at any instance flight
(u, v, w), the three aptitude angles (, Ψ, ϕ), the three angle of velocity vectors with
respect to the body axis coordinate system (α, β, γ), the aircraft position with respect
to the inertia reference (x, y, z), while the other six parameters are related to the
derivatives quantities in translational motion and rotational motion [13]. These flight
variables are all related to each other through a number of equations known as the
governing equations of flight motion and they belong to the class of non-linear time-
varying ordinary differential equation. Hence, the ability to solve the governing
equations of flight motion is important since it offers the capability to analyze the
flight dynamics behavior for any given type of aircraft. Therefore, the combination
with the control theory offers the possibility to define the behavior of an aircraft
during flight.
1.3 Objectives
The purpose of the present study is to develop the computer code for allowing user to
carry out flight dynamic analysis and flight control design. The input data for the
developed computer code are: i) the aircraft geometries, ii) mass and moments of
inertia properties of the aircraft and iii) flight conditions data. Hence, the present
work involves:
(a) The development of estimation for the primary aerodynamic characteristics
and the aerodynamic derivatives.
(b) The development of the procedure for solving trimmed flight.
(c) The development of the manners of solving aircraft flight motion in
longitudinal and lateral directions in their linear as well as in their nonlinear
form.
(d) The capability to be used as a controller design to allow the aircraft to have a
particular flight behavior with a PID controller.
6
1.4 Scope of work
The present work focused on the development of computer code for the flight
dynamic analysis and flight controller design of the fixed wing flying vehicle. Such
work will involve three scope of works namely i) aerodynamic characteristic
estimation, ii) the solution of flight dynamic equation of motion and iii) flight
controller design. These three scopes of works are carried out sequentially as shown
in the flow diagram as shown Figure 1.2 and can be explained as follows
(a) The first scope of aerodynamics characteristics will concern with the
aerodynamic estimation by use a semi empirical aerodynamics estimation
follows the method adopted from DATCOM [14], Ref [15] and Ref [16].
(b) The second scope concerned with deriving the governing equation of flight
motion in general form, trimmed flight, and their linearized form in
longitudinal, lateral and directional flight direction. In this scope of work will
involve in manner how to solve the trimmed flight equation, longitudinal
flight equation, lateral and directional flight equation and the nonlinear flight
equation by use of Simulink.
(c) The third scope related in the manner how to control flight behavior through
the operation of the three control surfaces (elevator, aileron and rudder) and
the engine thrust by use of PID controller scheme.
(d) The scope of work as stated in a, b and c will be converted into computer
code written in MATLAB programming language.
The developed software as stated in d was applied to five fixed-wing subsonic
aircraft models, namely are: Cessna 182 [17], Cessna 310 [18], Piper Cherokee 28-
161 [19], Learjet 24 [20] and Cessna 620 aircrafts [21]. The first three aircrafts
belonged to the class of propeller piston engine aircraft, while the last two aircrafts
were a turbojet and a turboprop engine type of aircraft respectively.
7
Software Required
Input Data
Mass and Moments of Inertia
Aircraft mass. Moment of inertia z-axis.
Moment of inertia x-axis. Moment of inertia xz-axis.
Moment of inertia y-axis.
Estimates Primary Aerodynamic Characteristics
CLo, Cmo, CLα,Cmα
, CLq, Cmq, CLα , Cmα
, Cyβ, Clβ, Cnβ , Cyp, ClP, Cnp,
Cyr, Clr, Cnr, CLδE, CmδE
, CyδA , ClδA
, CnδA, CyδR
, CnδR, ClδR
.
Perform believability
Coefficient Typically Coefficient Typically Coefficient Typically
Weight + Ixx + Izz +
Mass + Iyy + Ixz +
Ac of gravity 32.2 Wing span + Wing area +
Mean chord + CDmin 0.02 to 0.03 CDmin(point)
0.0
CLo 0.0 to 0.50 CLα 3.0 to 6.0 CLδ𝐸 0.3 to 0.9
CLα 1.0 to 8.0 CLq 4.0 to 10.0 Cyβ -0.3 to -1.0
CyδA <5.0 % of CyδR
CyδR 0.1 to 0.2 Cyp 0.0 to - 0.3
Cyr 0 .2 to 0.5 Clβ - 0.09 to - 0.30 ClδA 0.05 to 0.2
ClδR 0.0 to 0.02 ClP - 0.30 to - 0.6 Clr 0.07 to 0.20
Cmo - 0.056358 Cmα
- CmδE - 1.0 to – 2.0
Cmα – 3.0 to – 15.0 Cmq
- 11 to – 30 Cnβ 0.06 to 0.2
CnδA <10 % of CnδR
CnδR -0.06 to -0.12 Cnp -0.02 to -0.2
Cnr - 0.09 to -0.4
Yes
Start
Given Aircraft Configurations
Wing Surface Area. Mean Aerodynamic chord.
Wing Span. Other Geometric data.
Given Aircraft Flight Conditions
Flight altitude. True airspeed.
Mach number. Dynamic pressure.
Location of CG in % MAC. Steady-state angle of attack.
No
Dimensional Stability and Control Derivatives
Xu, Xα, XTu , XδE , Mα,, Mu, MTα, MTu
, Mα , Mq, MδE, Zu, Zα, Zα , Zq, ZδE,
Lβ, Lp, Lr, LδA, LδR, Nβ, NTβ, Np, Nr, NδA, NδR, Yβ, Yp, Yr, YδA, YδR.
Aero
dy
na
mic
Evalu
ati
on
s
8
Figure 1.2: Flight dynamics analysis and design procedure
Con
trol
Des
ign
Controller Flight Dynamics Behavior
Roll
Control
Yaw
Control
Pitch
Control
END
Method
I
Method
II
Simulink
Approach
State Space
Approach Transfer Function
Approach
Check via Routh - Hurwitz
Non-Linear Simulation Linear Simulation
Continued
Longitudinal Analysis
Lateral Analysis
Both
Yes
No
Transfer Function and
State-Space Approach
Comparison.
Linear and Non-Linear
Simulation Comparison.
Flight Dynamics Behavior
PID
SISO Control
Design
Control Design
PID
Conventional
Control Design
Fli
gh
t D
yn
amic
Eval
uat
ion
s
Trim Flight Analysis
Estimate trim lift coefficient. Estimate trim drag coefficient.
Estimate trim angle of attack. Estimate the trim angle of elevator.
Estimate the engine thrust at trim. Estimate the pitching moment
coefficient at trim.
9
1.5 Research methodology
In order to develop the capability in evaluating the flight dynamics in aircraft
behavior and the ability to design a controllable flight behavior upon a particular
flight variable, the proposed research methodology comprised of the following items:
(i) Literature research.
(ii) Procurement and commissioning of language program software.
(iii) Collecting aircraft geometry data and estimating the aerodynamic
characteristics needed in the equation of aircraft flight motion.
(iv) Solving the governing equation at trimmed flight condition.
(v) Solving the governing equation of flight motion in their linearized form.
(vi) Solving the governing equation of flight motion in non-linear aircraft model
by using a Simulink
(vii) Controller design under longitudinal flight mode.
(viii) Controller design under lateral and directional flight modes.
The validation of each scope work in view of aerodynamics estimation are carried by
comparing their result with the result provided by Ref [15] and [16], while in the
relationship with the solution of equation of the flight motion are validated with the
result provided by Ref [22]. In the control design with result adopted from Ref [23].
1.6 The results of the research work
The output of this research work had been in the form of software, which allows one
to evaluate the flight dynamic behavior and the controlling flight behavior for a
particular flight parameter. The software possessed the following capabilities:
(a) For a given aircraft configuration and flight condition, the software produced
primary and derivatives aerodynamics characteristics.
(b) In addition to the given mass and the moment of inertia, the software
produced the trimmed flight condition.
(c) Beginning with trim condition, the software evaluated the longitudinal and
the lateral – directional aircraft behavior based on linear flight equation.
10
(d) Beginning with trim condition, the software evaluated all flight parameters
that described the overall flight behavior by solving the non-linear governing
equation of the flight motion.
(e) For a particular flight parameter, the software had been able to be used as a
design tool for longitudinal or lateral–directional flight motion.
Considering the capabilities of the developed computer code as listed above, this
software may very useful in the development of the Unmanned Aerial Vehicle
(UAV) systems which currently had been attracted by almost all countries around
the World to have them. This system can be developed from the Remotely Controller
Aircraft (R.C Aircraft) in which such kind aircraft models are easily obtained in the
market.
1.7 Organization of the thesis
This thesis is divided into five chapters. The first chapter describes the introduction
chapter, including the problem statement, purpose objectives, scope of work, the
research methodology, the results of the research work and the organization of the
thesis.
The second chapter provides the literature review; this chapter is divided into eleven
sections. The first and second sections discuss the aircraft flight dynamics in general
and its governing equation of flight motion. The third section discusses the simplified
forms of the governing equation of flight motion in the form of equation known as
longitudinal equation and lateral-directional equation. The fourth section discusses
the governing equation of flight motion at trim condition. The fifth section
discusses the flying and handing quantities in view of longitudinal motion as
well as in the lateral-directional motion. The comparison between linear and
non-linear equation is discussed in the sixth section. Meanwhile, the seventh
section provides an overview in manner of the governing equation of flight
motion to be solved numerically by the use of numerical integration methods. The
eighth section describes an overview on controlling the aircraft movement
through the control surfaces that are used to influence the aircraft motions. The
ninth section discusses the aircraft control design and it reviews the PID
controller design. Finally, the last two sections discuss the flight dynamic
11
software; the tenth section describes the flight dynamic software in general and
the section eleven provides the examples of flight dynamic software that had
been developed in the past.
Chapter three of the present thesis describes how the flight equations of motions are
solved and the manner of controlling the aircraft movement. Hence, this chapter
includes the reviews on the research methodology that will be carried out,
aerodynamic characteristics estimations, and also the manner of the dimensional
stability and control derivatives to be determined. In addition to this, the solution of
flight motion based on transfer function, state space formulation and the three PID
controller design methods are discussed. Besides that, the non-linear aircraft
simulations are also presented in this chapter.
The results and discussions are presented in chapter four. It starts from describing the
aircrafts geometry, flight condition and mass and moments of inertia data of the
aircraft under investigation. This chapter is divided into three sections. The first
section is related to the longitudinal and lateral directional dynamic stability analysis
with or without control surfaces in operation. Here, for the given aircraft data, one
can evaluate how the flight variables such as aircraft speed u, angle of attack α, pitch
angle θ, change with respect to time in corresponding to the longitudinal motion.
Flight variables are in terms of the side slip angle β, the Euler roll angle ϕ and the
Euler yaw angle ψ with respect to time in relation with lateral motion. These various
flight variables are evaluated for different aircraft models. The second section
discusses the controller design. It reviews the PID controller design applied to a light
propeller aircraft model Cessna 182. The third section discusses the implementation
of the non-linear aircraft simulation developed by using Matlab Simulink. The
nonlinear aircraft simulation is applied to a propeller aircraft Piper Cherokee PA 28-
162. The last chapter which is chapter five provides conclusions and
recommendations for future research and references. This thesis is also accompanied
with three appendixes, A, B and C. Appendix A contains the manner of how
aerodynamics characteristics can be estimated based on the geometry data of the
aircraft. Appendix B describes the examples of how to implement the semi-empirical
aerodynamics method into the Matlab software. Appendix C describes the list of
publication that had been published during the time that the research work was
conducted.
CHAPTER 2
LITERATURE REVIEW
2.1 Aircraft flight dynamics
Flight dynamics is a branch of basic science of aeronautics that studies the flight
behaviors of the aircraft during the flight in an atmosphere. This field, which is
studied together with aerodynamics, aircraft structure and propulsion, plays an
important role in the activities of designing a new aircraft [24]. The flight dynamics,
as well as aerodynamics, represents a larger field of study. As a result, this field of
study is normally split into 5 fields, as suggested by Hull [25]. They are i) trajectory
analysis (performance), ii) stability and control, iii) aircraft sizing, iv) simulation and
v) flight testing. Besides, Etkin [26] provides some examples of the main type of
flight dynamics problems that occur in engineering practices, which are:
(a) Calculation of quantities performance, such as maximum flight speed, flight
altitude, flight endurance, fuel consumption, takeoff, and landing distance.
(b) Calculation trajectories, such as lunch, reentry, orbit, and landing.
(c) Stability of motion.
(d) Response of the vehicle due to control activation and due to propulsive
change.
(e) Response to atmospheric turbulence and how to control it.
13
(f) Aero elastic oscillation (flutter).
(g) Assessment of human–pilot/machine combination (handling qualities).
Considering the types of problems mentioned above, the first two types of the
problems can be categories as flight performance analysis. The scope of work
involved in this analysis is quite a formidable task, as asserted by Ojha [27] that a
performance analysis needs to be carried out for almost all phases of a flight, starting
from takeoff, climb, cruise, turn, descent, and finally landing. In each phase of a
flight, the aircraft may experience engine failure, so the aircraft flies at an unpowered
flight or at a gliding flight condition. In addition to this, the performance analysis
depends on the type of propulsive unit used with the specific types of aircraft.
On top of that, referring to the phases of aircraft flight at takes off, the speed of the
aircraft is quite low and in order to leave the ground, the aircraft has to be set in such
manner to generate lift greater than its weight. In cruise, the aircraft operates at a
constant speed and constant lift. Finally, when the aircraft lands, it needs to reduce its
speed without losing too much lift. Hence, the issue for control of the aircraft is how,
at a given speed, the incidence angle can be maintained. At take-off or landing, in
order to change the incidence of the wing, the aircraft will be rotated in nose up or
nose down. The aircraft control, in this respect, will study how the pilot can fix the
relationship between speed and incidence without increasing or losing too much lift.
In other cases, when an aircraft is in a cruise flight, in which the aircraft is at constant
speed and incidence while the control surfaces are kept at a fixed setting, here, the
aircraft stability needs to be identified in order to evaluate how an aircraft responds
to small disturbances in flight, as well as how it can be designed so that it can remain
at a fixed incidence and speed without overworking the pilot. Basically, there are
various improvements in other areas involved in designing a new aircraft; whether in
the point of aerodynamics, aircraft structure or propulsion system, as well as avionic
and aircraft systems. Compared to other transportation vehicles, aircraft has been
known as a product of high technology and cost, and also highly competitive
amongst the aircraft manufacturer industry. Although the aircraft manufacturer is
currently dominated by the European and the USA, their revenue is formidable. The
total commercial aircraft industry revenue for 1997 was approximately $ 60.0 billion,
of which $ 40.0 billion was attributable to U.S producers. As a result, the U.S aircraft
manufacturers contributed among the largest net exports to U.S governments, with
trade surpluses averaging about $ 25.0 billion annually over the early 1990s [28]. In
14
overall, the aerospace industry, which includes military aircrafts and missiles, based
on the results of market survey conducted by Boeing aircraft, manufacturer provides
the revenue for aerospace industry from 2010 to 2020 at an amount of $ 3.60 trillion
or yearly at around $ 180 billion [29]. Besides, the driving force in utilizing the flight
dynamics knowledge may come from the development of aircraft for fulfilling the
military purposes. Moreover, the ability to fly at a high angle of attack or at a higher
speed and better maneuverability solve a lot of issues related to flight dynamics. In
the past, building an aircraft with good stability characteristics that usually ensure
good flying qualities can only be achieved with good aerodynamic design.
Furthermore, in line with the development of automatic flight control systems
(AFCS), provision of good flying qualities is no longer a guaranteed product in good
aerodynamic design and good stability characteristics. This suggests that the study
pertaining to flight dynamics should be presented in a new format; from conventional
flight dynamics study to modern flight dynamics study. In this format, the modern
flight dynamics is concerned not only with the dynamics, stability, and control of the
basic airframe, but also with, sometimes, the complex interaction between airframe
and flight control system. At present, the modern flight dynamists tend to be
concerned with the wider issues of flying and handling qualities rather than with the
traditional, as well as more limited issues of stability and control. As a result, the
modern flight dynamics, as suggested by Cook [30], involves the work of:
(a) The establishment of a suitable mathematical framework for the problem, the
development of the equations of motion, the solution of the equations of
motion, investigation of response to controls, and the general interpretation of
dynamic behavior.
(b) Reviewing on contemporary flying qualities requirements, as well as their
evaluation and interpretation in the context of stability and control
characteristics.
(c) The development of the feedback control if an aircraft has unacceptable
flying qualities.
Therefore, the present work shared the scope of work suggested by Cook [30], as
mentioned above. Besides, the interest in dealing with problems concerning flight
dynamics; whether the problem in hand is related to the solution of flight
performance or flight stability, as well as control or flight simulation, they share
similar starting points as they start from the governing equation of flight motion.
15
Hence, further difference among of them in imposing the assumptions, which of
course will give a different form of governing equation of motion and how the
governing equation of the corresponding equation should be solved, had been looked
into. Thus, the governing equation of flight motion is presented in the following sub
chapter and in sequence manner, followed by the simplification of the governing
equation of flight motion, for the flight dynamics problem to be treatable.
2.2 The governing equation of flight motions
In flight, an aircraft can move in six degrees of freedom. The movement of the
aircraft can take in three translational and three rotational movements. In order to
understand the aircraft flight behavior, as well as to control the aircraft movement,
one has to derive the governing equation of flight motion. This governing equation
can reflect the possibility to determine the aircraft position, orientation, velocity,
acceleration, forces, and moment acting on the flying vehicle. Unfortunately, all
those quantities cannot be presented by just using a single coordinate system, as one
needs to use more than coordinate systems. Moreover, specifying the position and the
vehicle orientation requires one to define an inertial frame of coordinate system,
while for the forces and the moments that act on the vehicle may be referred to the
axis system attached to the flying vehicle. Strictly speaking, two coordinate systems
need to be defined in formulating the governing equation of flight motion, and they
are: i) the inertial coordinate reference system, and ii) the coordinate body fixed axis
reference system. The inertial coordinate system is defined as a system coordinate, in
which the Newton’s second law is applied [31].
In respect that the rotation of the Earth is relatively slow compared to the problems
involving the dynamics of aircraft, the Earth can be selected as the inertial coordinate
system of reference. Here, the selected coordinate system must be orthogonal and
right-handed [32]. Basically, defining the inertial coordinate system on the Earth can
be done in various manners; here, one can place the origin of the coordinate system
at anywhere on the Earth. Let the coordinate system be denoted by the symbol (F)
with a subscript intended to mnemonic the name of the corresponding coordinate
system. If it is so, (FI) reflects the coordinate system of inertial frame. Meanwhile,
the origin of the inertial coordinate system is denoted by symbol (OI) with the axes of
16
the system labeled as (x, y, and z) and the companion with an appropriate subscript
(I), they become (xI, yI, and zI). The unit vectors, along with x, y, and z, are denoted
as (i, j, and k) respectively. Besides, with the earth being selected as the place of an
inertial coordinate system, it had been identified that three models of the inertial
coordinate system are commonly used in solving the flight dynamic problems, which
are:
(a) The Earth-centered reference frame, (FEC), as shown in Figure 2.1a.
(b) The Earth-fixed reference frame, (FE), as shown in Figure 2.1b.
(c) The local-horizontal reference frame, (FH), as shown in Figure 2.1c.
(a) (b)
(c)
Figure 2.1: The locations of the origin of the coordinate systems [33]
17
Figures 2.1a, b, and c illustrate the placements of their origin of the coordinate
systems for the above three types of inertial coordinate systems.
If one chooses one of those three reference frames as its inertial coordinate axis
system, one has to be consistently used in the whole process of solving the flight
dynamics problems. However, it had been identified that most of the flying vehicles
in the atmospheres, as far as the flight speed below the hypersonic speed, a local
horizontal reference frame is preferred [34].
Meanwhile, the second coordinate system, besides the inertial coordinate system, is a
body fixed axis reference system. This coordinate system, assigned to have the origin
and the axes of the coordinate system, is fixed with respect to the geometry of the
aircraft. Here, three types of body fixed coordinate systems can be applied, and they
are:
(a) Body axis fixed coordinate systems.
(b) Stability axis fixed coordinate systems.
(c) Wind axis fixed coordinate systems.
These three coordinate systems are used in the aircraft’s center of gravity (C.G) as its
origin, and in defining the y and the z axes, they share the same orientation. Their
difference occurs in terms of defining the orientation of the x-axis, as depicted in
Figure 2.2. The x-axis of body axis fixed coordinate system normally coincides or is
parallel to the axis of fuselage. Meanwhile, the x-axis of stability axis fixed
coordinate is parallel with a line drawn to indicate that the present aptitude of aircraft
makes an angle of attack α to the incoming air velocity, whereas the x-axis of wind
fixed coordinate system has direction parallel to wind vector velocity defined with
respect to the x-axis of body axis fixed coordinate system. The choice of which one
will be used depends on the problem of flight dynamics that will be solved.
18
Figure 2.2: The orientation of body axis, stability axis, and wind axis [34]
In respect to the inertial frame of reference, the orientation of body axis coordinate
system is shown in Figure 2.3. In addition, forces and moments, as well as the
definitions of linear and angular velocities on the body axis are shown in Figure 2.4.
Figure 2.3: Body axis coordinate system [33]
19
(a) (b)
Figure 2.4a: Definitions of aerodynamic forces, thrust and acceleration gravitation in
body axis coordinate system [34]
Figure 2.4b: Definitions of moments, linear, and angular velocity in body axis
coordinate system [33]
The definitions of notations that appear in the above figures are explained in Table
2.1.
20
Table 2.1: The definitions of notations in describing forces, moment, and velocity
components [34]
NO DEFINITION ROLL AXIS xb PITCH AXIS yb YAW AXIS zb
1 Angular rate p q r
2 Velocity components u v w
3 Aerodynamic force components X Y Z
4 Aerodynamics moment components L M N
5 Moment of inertia about each axis Ixx Iyy Izz
6 Product of inertia Iyz Ixz Ixy
7 Engine thrust T ….. …..
Basically, the governing equation of flight motion can be broken down into two
groups [31]. The first group is the governing equation of flight motion derived from
the implementation of the Newton’s second law to the aircraft. Meanwhile, the
second group of equations is developed based on the kinematic relationship between
the inertial axis reference systems and the body fixed reference system [35].
As mentioned previously, the inertial coordinate system is employed to specify the
aircraft position, orientation, velocity, and the aircraft acceleration. In other words,
this inertial coordinate system allows one to apply the Newton’s second law to the
aircraft. If the aircraft mass is denoted as (m); the aircraft with respect to the inertial
reference system moves in varying directions based on the vector velocity , and
the forces acting on the aircraft ( ), hence, the Newton’s second law states that for
the given force ( ), there is equal time rate of change in its linear momentum .
Meanwhile, if represents the external moment applied on the aircraft, the
moment will be equal to the time rate of angular momentum . These two
statements can be written mathematically as:
(2.1a)
(2.1b)
The vector velocity represents the vector velocity of the aircraft center of gravity
measured with respect to the inertial reference frame, and the angular velocity vector
is denoted as . If the inertial reference axis is denoted as (XYZ) coordinate
system, while for the body fixed reference frame is denoted in small letter as (xyz),
21
hence the term
|
can be written in terms of
|
by using the
following relation:
|
|
| | (2.2a)
In a similar manner, the rate change of angular momentum, which was previously
written with respect to inertial coordinate system, then completely can be written
with respect to the body fixed coordinate in the following relation.
|
|
| | (2.2b)
Equation 2.2 is substituted to Equation 2.1; which gives the representation of the
Newton’s second law in body fixed reference frame as:
|
|
| | (2.3a)
|
|
| | (2.3b)
If the vector unit of the body axis system (xyz) for x-axis is denoted by , y-axis is
denoted by , and z-axis is denoted with its unit vector , and hence, the two
vectors, velocity ( and angular velocity ( , can be equated as:
(2.4a)
(2.4b)
The externally applied aerodynamic forces , and moments that act on the
aircraft are primarily due to airflow condition and their control surface deflections. In
a similar manner with vector velocity and vector angular velocity , this
applied force and moment , as well as angular momentum ( , can be broken
down into vector components along the longitudinal (x), the lateral (y), and the
vertical axis (z) of the body fixed reference frame. Besides, the force components in
the longitudinal, lateral, and vertical axes are denoted as (Fx), (Fy), and (Fz)
respectively. During application, the moment is denoted in terms of its
component as (L), (M), and (N). On the other hand, the vector angular momentum
associated with their components in body fixed reference is denoted as (Hx),
(Hy), and (Hz). Hence, the forces and the moments, as stated in Equations 2.1a and
2.1b, are written in the form of scalar notation as:
(2.5a)
22
(2.5b)
(2.5c)
(2.6a)
(2.6b)
(2.6c)
The vector angular momentum , in conjunction with the vector angular
velocity , can be written as:
[
] (2.7)
In assuming that the aircraft mass (m) is a constant and by substituting Equation 2.7
into Equations 2.5 and 2.4, one can write these two equations in scalar form as:
(2.8a)
(2.8b)
(2.8c)
( )
(2.9a)
(2.9b)
( )
(2.9c)
The left hand side of the above equations represents the external forces and moments.
These forces and moments are due to aerodynamic forces, aircraft weight, and engine
thrust, which can be written in the following forms:
(2.10a)
(2.10b)
(2.10c)
As for the moments, they can be written as in the following:
(2.11a)
(2.11b)
(2.11c)
23
The definitions of notations that appear in the right hand side of Equations 2.10 and
2.11 are given in the list of symbols.
In other forms, the force equations (Equation 2.10) can be written as:
(2.12a)
(2.12b)
(2.12c)
Meanwhile, the momentum Equations (Equation 2.11) can be written as:
( )
(2.13a)
(2.13b)
( )
(2.13c)
Furthermore, in a relationship between a body axis fixed coordinate system and the
Earth-fixed reference frame, the rotational velocity with respect to the body axis
fixed coordinate system is described by the variables (r, p, and q), while the Earth
fixed coordinate system is described by ( , , and ). The relationship between
these two triples is shown in [31]:
[ ] [
] [
] (2.14)
The above relationship indicates that if the body axis fixed coordinate system is
placed parallel to the Earth fixed coordinate system, which means (θ = 0.0 and ϕ =
0.0), one will obtain ( , and ). Hence, they show the angular rate of
the vehicle to the inertial frame of reference. Besides, the above equation (Equation
2.14) can be solved to represent how the aptitude of the flying vehicle changes with
the inertial frame of reference by inversing that equation and provides the result as:
[
] [
] [ ] (2.15)
Meanwhile, the aircraft position with respect to the inertial reference frame at any
instant results in:
24
[
]
[
] [ ] (2.16)
Equation 2.12 to Equation 2.16 represents the governing equation of aircraft flight
motion. These equations contain 12 state variables, which are sufficient in describing
the flight behavior of the aircraft.
In addition to these 12 state variables, one may add three other state variables: i) the
total velocity (V), ii) the angle of attack α, and iii) the side slip angle β. These three
state variables can be derived from the component velocities (u, v, and w) as depicted
in the following:
√ (2.17a)
(
) (2.17b)
(
) (2.17c)
If one applies the first derivative with respect to time into these three above
equations, one can obtain:
(2.18a)
(2.18b)
( )
√ (2.18c)
If , and , which are defined by Equation 2.12, are substituted into the above
equations, the results are:
(2.19a)
(2.19b)
(2.19c)
With the definitions of (Fx, Fy, and Fz), as given by Equation 2.10 into Equation 2.19,
one obtains the state variables (V, α and β) as:
(2.20a)
221
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