Flight Dyanamic

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    CHAPTER 1

    INTRODUCTION

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    1.1 General

    Interest in unmanned-aerial-vehicles (UAVs) and micro-aerial-vehicles (MAVs) in

    recent years has increased significantly. These aircraft are useful for applications ranging

    from military to scientific research because of their ability to perform dangerous missions

    without risking human life. Also because their payload can be much smaller than a pilot,

    there are less limitations to how small they can become. At Brigham Young University (BYU)

    in particular, small UAV research has exploded during the last few years. Faculty and

    students work together on many small UAV projects. Research activities include developing

    new airplanes for commercial use, participating in the annual Micro-Aerial-Vehicle

    competition, and developing autonomous flight vehicle systems. It seems that interest in

    small UAVs will continue to grow around the world as new applications will demand new

    UAV solutions and designs. Airplanes come in all shapes and sizes. Before the emergence of

    UAVs, airplane designers were constrained in how small they could go because of the

    necessity to carry a human pilot onboard. By removing the pilot, and due to increasing UAV

    component technology, UAV designs have decreased in size significantly. As time goes on,

    smaller and smaller UAV solutions will become available. Indeed, the term small UAV

    undoubtedly had a much different meaning just a few years ago than it does now.

    Small, remotely operated aircraft present unique challenges and advantages to both

    designer and pilot. Because of a drastically higher crash frequency, it seems that small UAVs

    are more susceptible to dangerous and sometimes fatal instabilities than large airplanes.

    This may be due in part to quicker design cycles and the lower stakes of small UAV crashes

    relative to the high stakes of a large airplane crash. Perhaps designers are sometimes

    more eager to get out and see if this thing flies, than they are to do the rigorous design

    work necessary to ensure a stable and successful first flight. Often, experienced airplane

    designers and pilots seem to develop an uncanny intuition for diagnosing and solving

    problems with all kinds of airplane instabilities. The goal of this thesis research is to capture

    the intuition and knowledge of such capable engineers and pilots, evaluate it quantitatively

    and provide a simple tool to new, less-experienced designers. This tool will allow them to

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    improve their small UAV design methods to include considerations of both static and

    dynamic stability.

    Airplanes, including small UAVs, are a classic engineering example of design

    tradeoffs. It often seems impossible to improve one aspect of performance without

    degrading another. Accordingly, stability is one aspect of airplane performance that must be

    balanced with all the others. There are two types of stability which are:

    Static Stability

    Static stability is an essential part of the basic airplane design process already included indesign methodologies.

    Dynamic Stability

    Dynamic stability will effect on performance and handling qualities is generally poorly

    understood by new designers. This lack of understanding makes it difficult to include

    dynamic stability into a typical design process.

    An airplane that has positive dynamic stability does not automatically have

    positive static stability. The designers may have elected to build in, for example, negative

    static stability and positive dynamic stability in order to achieve their objective in

    maneuverability. In other words, negative and positive dynamic and static stability may be

    incorporated in any combination in any particular design of airplane.

    An airplane may be inherently stable, that is, stable due to features incorporated in

    the design, but may become unstable due to changes in the position of the center of gravity

    (caused by consumption of fuel, improper disposition of the disposable load, etc.). Stability

    may be (a) longitudinal, (b) lateral, or (c) directional, depending on whether the disturbance

    has affected the airframe in the (a) pitching, (b) rolling, or (c) yawing plane.

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    Figure 1.2: Stability diagram

    This research will provide relatively simple methods to approximate the static

    behaviour and handling qualities of small UAVs while still in the design stage, similar to

    analysis used in a conventional large aircraft design process. In the future, this will hopefully

    become a powerful tool in the hands of small UAV designers at BYU and elsewhere. Perhaps

    in the future it will be possible to avoid fatal crashes like that shown in Figure 1.1

    Figure 1.1 Damage from small UAV crashes like this one often result from a lack of

    designing for stability.

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    1.2 The Objective of This Study

    The objective of this thesis research is to better understand aircraft static stability as it

    applies to small UAVs and to develop a method for including static stability analysis into the

    design process. This objective can be broken down into four sub-objectives which will be the

    topics covered in this thesis:

    Develop a mathematical model to predict the static stability of small UAVs based on

    knowledge of the geometry and inertias of the airframe.

    Verify the accuracy of the model using known airplane data.

    Provide analysis of the driving design parameters and guidelines for small UAV

    static stability.

    1.3 Stability: A Requirement for All Airplanes

    Among the significant but often-overlooked obstacles to powered flight overcome by

    the Wright brothers was the question of how to build an airplane that was stable enough to

    be controlled and manoeuvred by a pilot. It has been shown that the Wrightsfirst powered

    airplane in 1903 was so unstable that only the Wrights themselves could fly it, due to

    extensive self-training on their previous glider versions in 1902. (Abzug, 3) As they and other

    aviation pioneers took steps to solve the stability and controls problem, the capabilities and

    performance of airplanes increased significantly. In the early days of flight, it was observed

    that certain designs of airplanes were more stable and controllable than others, but it was

    not until the 1930s that much theory existed to explain why. Much of the modern stability

    and control theory and specifications were not developed until the 1960s or later. (Abzug,

    33) Airplanes of all sizes must be capable of stable, trimmed flight in order to be controllable

    by a human pilot and useful for various applications. Stable flight by a human pilot is

    possible only if the airplane possesses static stability, a characteristic that requires

    aerodynamic forces on the airplane to act in a direction that restores the plane to 12 a

    trimmed condition after a disturbance. Dynamic stability requires that any oscillations in

    aircraft motion that result from disturbances away from equilibrium flight conditions must

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    eventually dampen out and return to an equilibrium or trimmed condition. Certain

    dynamic instabilities can be tolerated by a human pilot, depending mostly upon pilot skill

    and experience. If computer-augmented feedback control is used even statically unstable

    aircraft can be flown successfully. (Abzug, 312) Both static and dynamic stability

    characteristics can be predicted while an airplane is still in the design stage of development.

    Many companies such as DAR Corporation, whose theory will be used extensively in this

    chapter, have developed software to do just that. (Roskam, I, 461) To do so, it is necessary

    to have a precise knowledge of the geometric and inertial properties of the airframe. Static

    stability is predicted using information about the airplane aerodynamic center and the

    center of gravity as well as other geometric parameters. Dynamic stability is predicted using

    the airframe geometric and inertial properties to calculate the natural frequencies, damping

    ratios and time constants of the characteristic dynamic modes of the six degree-offreedom

    aircraft model. The handling qualities of an airplane are said to be a measure of how well an

    airplane is able to perform its designated mission. They are usually evaluated using flight

    test data and pilot feedback on performance. Current military specifications relate levels of

    acceptable aircraft handling qualities to the frequencies, damping ratios and time constants

    of the dynamic modes.

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    1.4 Static Stability

    An airplane possesses static stability if the aerodynamic forces and moments

    introduced on the airframe as a result of it being disturbed from equilibrium tend to act in a

    direction that will return the airplane to an equilibrium condition. Static stability is

    analogous to a marble in a bowl. If the marble is disturbed from an equilibrium position at

    the bottom of the bowl, gravitational forces at all other positions will tend to pull it back

    towards the bottom. Aerodynamic forces and moments on a statically unstable aircraft will

    tend to move it away from a trimmed flight condition when it is perturbed from equilibrium.

    This condition is analogous to a marble on the top of a smooth hill or balancing a pendulum

    upside down. This condition would be nearly impossible for a human pilot to control, but

    could be possible if some form of feedback control is used. For a more complete overview of

    static stability, readers should consult Anderson, Chapter 7, in the References section. Static

    stability can be considered as a special case (steady-state) of the aircraft dynamics. It is

    exhibited in both the decoupled longitudinal and lateral-directional axes. It will also become

    clear that both longitudinal and lateral-directional static stability are a prerequisite for

    dynamic stability.

    1.4.1 Longitudinal Static Stability

    Longitudinal static stability is essential to ensure that a human pilot can successfully fly an

    airplane without stability augmentation. It depends mostly upon a parameter known as the

    static margin, defined as the distance between the aircraft center of gravity and the neutral

    point of the aircraft, normalized by the mean geometric chord, c , of the wing. An airplane

    with longitudinal static stability must first possess a positive (nose-up) pitching moment

    from the combination of the aerodynamic forces and moments on the wing and tail. For

    flying wings, an airfoil with a natural positive pitching moment must be chosen or washout

    and wing sweep must be combined to give the airplane a natural positive pitching moment.

    If this condition is met, a positive static margin, defined as the center of gravity in front of

    the neutral point, will ensure static stability. Static stability can be simply represented by

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    plotting the pitching moment of the aircraft about its center of gravity versus angle-of-

    attack as shown in Figure 2.1.

    Figure 1.1 A moment coefficient curve for an airplane possessing longitudinal static stability.

    Any disturbance away from trim will result in aerodynamic forces and moments which will

    act in a direction that will tend to return the plane to equilibrium.

    A small static margin (center of gravity near the neutral point) will provide marginal static

    stability and will be represented by a nearly flat line on the graph in Figure 2.1. A large static

    margin will provide a steep line and can make an airplane feel nose-heavy.It may cause

    the plane to be less controllable because it doesnt respond to control inputs. These

    constraints on the static margin are presented in Figure 2.2. It is also important that the

    static margin be chosen that will allow the plane to be trimmed at a reasonable angle of

    attack.

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    Figure 1.2 Aircraft center of gravity envelope. The c.g. must fall within these limits set by the

    stability and controllability of the aircraft. (Kimberlin, 2006).

    To express longitudinal static stability in mathematical terms, we must first define

    the aerodynamic centre, . It is the longitudinal location along the centreline of theaircraft measured from the leading edge of the wing about which the pitching moment is

    constant over a range of angles-of-attack. It is also the point at which the lift effectively acts.

    1.4.2 Lateral-Directional Static Stability

    Similar to the longitudinal case, an UAV possesses directional (about the z-axis or

    yaw-axis) static stability if a slight increase in sideslip results in a restoring yawing moment

    as well as a restoring side force. This is sometimes called weathervane stability. Lateral

    (about the x-axis or roll axis) static stability is expressed in terms of dihedral effect. If these

    are negative, then the airplane will possess positive lateral stability and will exhibit a

    negative rolling moment (left wing down) for a positive sideslip (nose left).

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    1.5 Dynamic Stability

    An UAV possesses dynamic stability if the amplitudes of any oscillatory motions

    induced by disturbances eventually decrease to zero relative to a steady-state flight

    condition. This means that if an UAV experiences a small perturbation from trimmed flight,

    it will eventually return to trim on its own. This is analogous to a marble in a bowl eventually

    coming to rest at the bottom of the bowl. If the amplitude of oscillatory motion instead

    tends to increase with time, the airplane is said to be dynamically unstable. Dynamic

    instabilities are obviously undesirable, but certain mild dynamic instabilities can be

    tolerated by a human pilot. If automatic controls are used, more severe dynamic instabilities

    can also be tolerated. Graphical representations of dynamic stability and instability are

    shown in Figures 1.3 and 1.4. To study dynamic stability, it is necessary to analyze the well-

    known differential equations of UAV motion. For small perturbations, these equations can

    be decoupled into longitudinal and lateral-directional portions, with 3 degrees of freedom in

    each. Small perturbation theory also allows us to approximate the actual non-linear

    equations as linear differential equations with constant coefficients while ignoring any less

    significant non-linear aerodynamic effects. This greatly simplifies the analysis of the dynamic

    modes of aircraft motion. However, it should also be explained that we will only considerthe static stability only in this study.

    Figure 1.3 A graphical example of dynamically stable UAV motion relative to a steady-state

    condition.

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    Figure 1.4 A graphical example of dynamically unstable UAV motion.

    1.6 Longitudinal Dynamic Stability

    The longitudinal dimensional stability derivatives represent the partial derivatives of

    linear or angular acceleration due to either the displacement, velocity or acceleration

    depicted by the subscript. The capital letters X, Y and Z represent derivatives of linear

    accelerations in the corresponding directions while the capital letters L, M and Nrepresent

    derivatives of angular accelerations according to the conventions. The dimensional stability

    derivatives are the dimensionalised form of the non-dimensional stability derivatives

    depicted by the letter C with appropriate subscripts. Both can be derived experimentally or

    analytically with a careful analysis of the airframe geometry and inertial properties. The

    variables u, , and are the perturbed velocity, angle-of-attack and pitch attitude

    respectively and represent the three longitudinal degrees of freedom. By taking the Laplace

    transform of this system, the differential equations become simple polynomials in the s

    variable and are transformed from the time domain into the frequency domain.

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    CHAPTER 2

    CALCULATIONS

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    Table 2.1 AirTRAC UAV Parameter

    NO PARAMETER VALUE

    1 Distance from leading edge

    to the chord of wing

    2 Distance from leading edge

    to the center of gravity 3 Wing root chord Croot= 0.16013m

    4 Wing tip chord Ctip= 0.11952m

    5 Mean chord length 6 Wing area 7 Wing aspect ratio

    9.22

    8 Wing lift curve slope 9 Wing taper ratio 0.7464

    10 Tail area 11 Tail aspect ratio 6.70612 Tail lift curve slope 2.40713 Distance from chord of tail

    to center of gravity

    m14 Tail efficiency 15 Tail volume ratio 0.42716 Length of fuselage 17 Fuselage body side area 18 Distance from nose to cg 19 Maximum width fuselage

    20 Vertical height of fuselage at

    length of fuselage 21 Vertical height of fuselage at

    length of fuselage

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    2.1 Pitching Moment

    2.2 Longitudinal static stability

    An equilibrium point can be stable, unstable or neutral stable. A stable equilibrium

    point is characterized by and . The criteria for longitudinal static stability canbe pictured as:

    Figure 2.1 Moment coefficient curve with negative slope

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    Figure 2.2 Moment coefficient curve with negative slope

    If the airplane is statically longitudinal stable, it has the initial tendency to return to its

    equilibrium position.

    For our analysis, the graph can be shown as:

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    Figure 2.3 CMcgversus of the AirTRAC UAV

    For the calculation of the trim angle it is given by:

    Neutral Point and Static Margin Determination

    To find the neutral point of the AirTRAC UAV, there is several assumption that have been

    made:

    i)

    based on the center of gravity

    based on the neutral point

    y = -0.944x - 0.0147

    -30

    -20

    -10

    0

    10

    20

    30

    -20 -10 0 10 20

    C

    oefficientofmoment,Cm

    Angle of attack,

    Cm versus

    TOTAL

    wing

    tail

    Linear (TOTAL)

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    ii) iii)

    Figure 2.4 Effect of the location of the centre of gravity relative to the neutral point on

    static stability

    Then, equation of the neutral point is given as below:

    ( )

    Component Method Weight

    (kg)

    x(mm) Wx

    (kgmm)

    Staticall Unstable

    Neutral Stabilit

    Staticall Stable

    trim

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    Fuselage Stinton 1.6 217.00 347.20

    Wing Stinton 2.4 241.20 578.88

    Payload Estimation 2.2 203.66 448.05

    Tail Stinton 0.4 885.43 354.17

    Fuel Estimation 3.4 275.05 935.17

    Powerplant Stinton 4.0 107.64 430.56

    Structure Stinton 5.4 276.89 1495.21

    Equipment and

    services

    Stinton 0.6 208.27 124.96

    Total 20.0 Total 4714.20

    Figure 2.5 The final location of components of the AirTRAC UAV and the weight

    Thus, based on the table above, we can calculate the location of the maximum,

    minimum, forward and after centre of gravity. The location of maximum centre of gravity is

    including the all components of AirTRAC UAV with the fuel in the tank

    The location of minimum centre of gravity is including all components with empty fuel of

    AirTRAC UAV

    Next, the static margin is defined as below:

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    The neutral point is located at aft the centre of gravity,. In other word, theallowable margin in shifting the neutral point is between 0.236 m to 0.436 m measured

    from the leading edge of the AirTRAC UAV.

    The pitching moment equation M, will determine the longitudinal static stability of

    an aircraft. The changes of pitching moment with angle of attack will determine the

    characteristics of the aircraft longitudinal stability. A longitudinal statically stable at An aircraft has a good controllability if it can be trimmed at the positive angle of

    attack, . For our aircraft by referring the equation of total coefficient of moment at center

    gravity, the value of which is less than zero. Thus it can be stated that our

    aircraft is statically stable. Besides the value of Cmo is 0.0147 which is more than zero. It

    made the aircraft can be trimmed at positive .

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    The location of centre of gravity is an important characteristic in order to determine

    the aircraft stability while in preliminary design. In order to achieve a good longitudinal

    stability, Centre of Gravity (CG) should be ahead of Neutral Point (NP), which is

    Aerodynamic Centre (AC) of the whole aircraft. NP is the longitudinal location of CG when

    the aircraft is neutrally stable. When CG is ahead of NP, the weight tends to correct the

    upset thus lead to stable aircraft. While when the CG is behind NP, the weight worsens the

    upset thus make the aircraft become unstable. NP is the most aft CG location.

    During operation the CG location is not fixed. So that it is important to know the limit

    and range of CG location. The determination of CG when is important to estimatethe margin of aircraft longitudinal static stability.

    is called stick fixed neutral point. For

    our UAV, the value of XNPis 0.272. When XCGis at XNP, aircraft is neutral stable.

    The location of centre of gravity closer to tail which means the aircraft has shorter

    tail moment arm, causes the aircraft to destabilize. The longer the tail moment arm, thehigher the pitching moment due to pitch rate, q and change in angle of attack, . Theaircraft pitching moment due to angle of attack, M changes with the location of CG and

    aircraft aerodynamic centre. The closer is the CG to the AC, the aircraft will pitch at higher

    angle of attack and it resulted in higher natural frequency. Not only it is significant in

    longitudinal motion of the aircraft, but the tail moment arm also affects the yawing and

    rolling moment of the aircraft due to yawing rate in lateral mode.

    2.3 Lateral static stability

    Since the UAV is used primarily for surveillance purposes, a higher degree of rolling

    stability is required in order for the UAV to provide a clearer picture of the surroundings.

    The higher the slope of the rolling moment curve, the higher degree of rolling stability the

    UAV will possess.

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    The main contribution to an aircraft's lateral stability is the dihedral of the wings that will

    create a restoring moment when the aircraft is disturbed about its lateral axis A dihedral of

    6 degrees is introduced to enhance the rolling stability of the aircraft. The effect of dihedral

    on can be calculated as follows:

    Since plain rectangular wings are used, the integration can be simplified to be:

    The aircraft's lift curve slope can be calculated using the following equation:

    ( ) ( )

    ( )

    In this calculation, fuselage contribution is neglected due to the fact that there is a

    relatively large gap between the fuselage and the wings which will reduce the effect of

    change in flow induced by the fuselage.

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    Figure 2.6 Lateral Stability

    As shown in Figure 2.6, the negative value of tells us that the aircraft is laterally stable.

    2.4 Directional static stability

    Contribution of wing and fuselage

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    There are two main contributions to the aircraft's directional stability, namely the fuselage

    and the vertical tail. The fuselage's contribution to the yawing moment slope can be

    determined as follows:

    Whereis the empirical wing-body interference factor determined by the geometry of thefuselage. The value of can be determined from Figure 2.7 using the required geometricparameters. The required parameters for determination of are summarized in the tablebelow:

    Table 2.2 Fuselage geometric parameter for determination of 0.5345 2.5658

    1.19

    1

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    Figure 2.7 Wing body interference factor

    Referring to Figure 2.7, the value of is determined to be approximately 0.005.

    The value is a correction factor that depends on the fuselage's Reynolds number,

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    Contribution of vertical tail

    The vertical tail contribution to the fuselage's directional stability can be determined as

    follows:

    ( )

    Where the term can be estimated as follows:

    ( ) = the distance parallel to the z axis from the wing root quarter chord to the fuselagecenterline= the max fuselage depth

    ( )

    ( )

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    The total aircraft's yawing moment slope is the algebraic sum of each contribution.

    1.8531rad-1

    For static directional stability, the slope of the yawing moment curve must always be

    positive,

    as shown in Figure 2.9 below.

    Figure 2.9 Static directional stability

    The positive value of the aircraft's yawing moment slope is 1.8531rad-1

    . It indicates that the

    aircraft is directionally stable.

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    CHAPTER 3

    HANDLING QUALITIES

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    3.1 Flying and Handling Qualities

    The handling qualities of an airplane are said to be a measure of how well anairplane is able to perform its designated mission. They are usually evaluated using flight

    test data and pilot feedback on performance. Current military specifications relate levels of

    acceptable aircraft handling qualities to the frequencies, damping ratios and time constants

    of the dynamic modes. It is an obvious fact that an airplanes geometric and inertial

    properties, among other factors, influence how well or how poorly it flies and how

    effectively it is able to perform its intended mission. The handling qualities or flying

    qualities of an airplane are a measure of airplane performance relative to its intended

    mission and describe how well or poorly a particular airplane flies.

    MIL-STD-1797A defines what is meant by the term handling qualities. Those

    qualities or characteristics of the aircraft that govern the ease and precision with which a

    pilot is able to perform the tasks required in support of an aircraft role. Another definition

    from the Cooper-Harper Rating Scale defines handling qualities as those qualities or

    characteristics of an aircraft that govern the ease and precision with which a pilot is able to

    perform the tasks required in support of an aircraft role. (Hodgkinson, 7). An analysis of

    handling qualities will include both qualitative and quantitative information about the pilots

    ability to control the airplane. It includes analysis of how quickly an airplane responds to

    various inputs as well as the control effort that must be exerted by the pilot. Handling

    qualities are used to compare various aircraft designs and are based on both subjective pilot

    opinion and objective flight data.

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    UAVs are unique in the sense that there are no set hard and fast rules for the

    employment. Mission and role dictate the general design requirements and small size with

    no human on-board makes the launch, recovery methods up to the imagination of the

    designer. Thus it is very difficult to classify and define all the methods, however, the general

    guidelines as given in are listed below. The mini UAVs / RPVs are considered to be a

    different class and the UAVs are categorized as Table 1 according to the weight and

    maneuverability levels. Similarly the flight phase categories and the levels of handling

    qualities are also defined in Tables 2 and 3.

    Table 1:Categories of UAVs

    Class Category Mission examples

    I Small Light Weight Mini RPVs

    II Low maneuvarability Surveillance, Reconnaissance high

    altitude

    III Medium maneuvarability Surveillance, Reconnaissance low

    altitude

    IV Highly maneuverability UCAVs

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    Table 2:Flight phase categories

    Category Definition Flight types

    A

    Requiring rapid maneuvering, precision

    tracking, and/or precise flight path

    control.

    Reconnaissance, Target

    Acquisition, Terrain Following,

    In-flight refuelling etc

    B

    Requiring gradual maneuvers, without

    precision tracking, although precise

    flight path control may be required.

    Climb, Cruise, Loiter, Decent,

    Aerial Delivery, Emergency

    climb and decent.

    C

    Launch Recovery Phase requiring rapid

    maneuvering, precision tracking, or

    precise flight path control.

    Arresting Gear Landings, Net

    Capture, Conventional take-off

    and landing

    D

    Launch Recovery Phase requiring

    gradual maneuvers, without precision

    tracking, although precise flight path

    control may be required.

    Catapult take off, Approach,

    Parachute Recovery, Approach

    to recovery envelop

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    Table 3:Levels of flying qualities

    Level Definition

    I (A/M) (Normal System Operation) Flying qualities are clearly adequate to

    accomplish mission flight phase

    2 (A/M) (Degraded Mission) Flying qualities remain adequate to perform

    mission flight phase with moderate degradation or increase in operator

    work load, a degradation of mission effectiveness or both

    3 (A/M) (Recoverability) Degraded qualities remains adequate to control the

    vehicle with Category A phases terminated successfully and Categories

    B, C, and D phases completed sufficiently to recover the vehicle

    A: Automatic Control Mode

    M: Manual Control Mode

    Or RPV mode

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    3.2 Cooper Harper Rating Scale

    The dynamics and characteristics of the aircraft are related to the flying and handlingqualities. The natural frequency and damping ratio value influence on how easy or difficult

    to control the aircraft. Cooper Harper rating scale is being used as a reference to give rating

    for the aircraft. The rating scale gives from 1 to 10 that will influence the flying and handling

    qualities to aircraft.

    Figure 1:A modified form of Cooper Harper scale for UAV evaluation

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    3.3 Handling Qualities of UAV

    Most of the military specifications are derived by setting limits on the natural

    frequencies, damping ratios and time constants of the various dynamic modes. For instance,

    in the longitudinal axes, the natural frequency and damping ratio of the Phugoid mode

    describe what aircraft motions occur when the airplane seeks a stabilized airspeed

    following a disturbance. Because the natural frequency of this characteristically slow mode

    of oscillation is typically on the order of 50-100 seconds for large aircraft, a pilot is easily

    able to control and compensate for unwanted motion. Therefore, no limits are placed on

    the natural frequency of the phugoid mode.

    However, Level 1 handling qualities require that the damping ratio be positive so as

    to eventually cause any oscillation to die out over time. Negative damping ratios are

    tolerated only at Level 3 because they indicate a tendency to become unstable if

    uncorrected. Similar requirements, putting limits on the natural frequency and damping

    ratio of the Dutch-roll mode as well as the time constants of the spiral and roll modes, exist

    for the case of lateral-direction handling qualities. For the spiral mode, no specific limitation

    is placed on the time constant because a slightly unstable spiral mode is typically

    acceptable. However, lower limits on the time it takes for the bank angle to double from an

    initial disturbance of 20 degrees are specified. For the case of a stable spiral mode, the bank

    angle will actually decrease after a disturbance.

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    Table 4:Short period damping ratio limits

    Level Category A and C Flight Phases Category B Flight Phases

    Minimum Maximum Minimum Maximum

    1 0.35 1.30 0.30 2.00

    2 0.25 2.00 0.20 2.00

    3 0.15* - 0.15* -

    Table 5:Phugoid damping ratio limits

    Phugoid mode

    Level 1 > 0.04

    Level 2 > 0

    Level 3 T2> 55s

    Table 6:Spiral mode (minimum time to double amplitude flying qualities

    Class Category Level 1 Level 2 Level 3

    I and IV A 12 s 12 s 4 s

    B and C 20 s 12 s 4 s

    II and III All 20 s 12 s 4 s

    Table 7:Roll mode (maximum roll time constant) flying qualities (in seconds)

    Class Category Level 1 Level 2 Level 3

    I, IVA

    1.0 1.410

    II, III 1.4 3.0

    All B 1.4 3.0 10

    I, IVC

    1.0 1.410

    II, III 1.4 3.0

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    Table 8:Dutch roll flying qualities

    Level Category Class Min *

    Min n*,

    rad/s

    Min n,

    rad/s

    1

    A I, IV 0.19 0.35 1.0

    II, III 0.19 0.35 0.4

    B All 0.08 0.15 0.4

    C

    I, II-C 0.08 0.15 1.0

    IV

    II-L, II 0.08 0.15 0.4

    2 All All 0.02 0.15 0.4

    3 All All 0.02 - 0.4

    Where C and L denote carrieror land-based aircraft

    *The governing damping requirement is that yielding the larger value of

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    CHAPTER 4

    DECLARATION OF APPROVAL

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    Declaration for Approval

    With a detailed research had done, we had come out with a solid design for our proposed

    UAV design for air traffic surveillance. The SolidWork drawing is a general idea picked from

    our group members idea that had the greatest score. So we really hope with the data and

    initial estimation that had been calculate will make you confident and let us proceed with this

    design.

    Proposed by:

    ____________________

    (NUR FATIN MOHAMAD IDRIS)

    _____________________

    (MOHD ZAMRI MHD NASIR)

    _____________________

    (NUR HAZIQAH BAROM)

    ____________________

    (AHMAD AMEER ABDULLAH)

    ____________________

    (MUHAMMAD HAIKAL ABDUL JAMAL)

    Approved by:

    ____________________

    (EN MD NIZAM B DAHALAN)

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    CHAPTER 5

    REFERENCES

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    1. Anderson, John D. Introduction to Flight Fourth Edition. McGraw-Hill International

    Editions, 1999.

    2. Nelson, Robert C. Flight Stability and Automatic Control - 2nd Edition . McGraw-Hill

    International Edition, 1998

    3. Anderson, John D.Aircraft Performance and Design. McGraw-Hill International Editions,

    1999.

    4. Raymer, Daniel P. Aircraft Design: A Conceptual Approach 2nd Edition. American

    Institute of Aeronautics and Astronautics,

    5. Tang Shiao Loong, Infantry Section Unmanned Aerial Vehicle (UAV) Flight Controls and

    TestingNational University of Singapore 2012