Ac Design Project 2
Transcript of Ac Design Project 2
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AIRCRAFT DESIGN PROJECTII
(MULTIROLE FIGHTER AIRCRAFT)
A PROJECT REPORT
Submitted by
Batch - 18
A. ARIF ABDUL RAHMAN 11908101701
P. SANTHOSH 11908101704
T.V.S SARAVANAN 11908101705
I n partial ful fi llment for the award of the degree
Of
BACHELOR OF ENGINEERING
IN
AERONAUTICAL ENGINEERING
VEL TECH (ENGINEERING COLLEGE)
ANNA UNIVERSITY: CHENNAI 600 025
OCTOBER 2011
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ANNA UNIVERSITY: CHENNAI 600 025
BONAFIDE CERTIFICATE
Certified that this project report titledAIRCRAFTDESIGN PROJECTII(MULTIROLE FIGHTER
AIRCRAFT) is the bonafide work of
A. ARIF ABDUL RAHMAN 11908101701
P. SANTHOSH 11908101704
T.V.S SARAVANAN 11908101705
who carried out the work under my supervision.
SIGNATURE SIGNATURE
Mr. G. BOOPATHY M.E., Mr. M. Ramakrishna M.E.,
HEAD OF THE DEPARTMENT INTERNAL GUIDEDept of Aeronautical Engg. Dept of Aeronautical Engg.
Vel Tech Engg. college Vel Tech Engg. college
No.42 , Avadi - Vel Tech Road, No.42 , Avadi - Vel Tech Road,
Chennai-62 Chennai-62
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CERTIFICATE FOR EVALUATION
College Name : 119 - VEL TECH ENGG COLLEGE
Branch : AERONAUTICAL ENGG.
Semester : VII
The reports of the project work submitted by the above students in
partial fulfillment for the award of Bachelor of Engineering degree In
Aeronautical Engineering of Anna University were evaluated and confirmed
to be the reports of the work done by the above students and then evaluated.
INTERNAL EXAMINER EXTERNAL EXAMINER
S.NO
Name of the Students
Who have done
the project
Title of the project
Name of the
Supervisor with
Designation
1.A. ARIF ABDUL
RAHMANMULTIROLE
FIGHTER
AIRCRAFT
Mr. M. Ramakrishna
M.E.,
Asst. Prof.,
Internal guide
2. P. SANTHOSH
3. T.V.S SARAVANAN
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ACKNOWLEDGEMENT
This project, though done by us would not have been possible, without thesupport of various people, who by their cooperation have helped us in
bringing out this project successfully.
We are grateful to our Chancellor, Dr. R. Rangarajan B.E (Elec), (Mech),
MS (Auto) for his patronage towards our project.
We thank our Principal I/c, Mr. E. Kamalanaban M.E., (Ph.D),who had
always served as an inspiration for us to perform well. We would like to
express our faithful thanks to our head of the department, Mr. G. Boopathy
M.E., for having extended all the department facilities without slightest
hesitation.
We would like to express our unbounded gratefulness to our internal guideand project incharge, Mr. M. Ramakrishna M.E., Asst. Prof., Dept of
Aeronautical Engg. For his extremely valuable guidance and encouragement
throughout the project.
We thank all faculty members and supporting staff for the help they
extended to us for the completion of this project.
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TABLE OF CONTENTS
1.0 Introduction to ADP-II
1.1 Three view drawing
1.2
Data from ADP-I
2.0 V-n diagram for design study
2.1 V-n diagram (Take off, cruise, landing)
3.0 Gust and maneuverability envelopes
3.1 V-n diagram (gust loads)
3.2 Final V-n graph calculation
4.0 Structural design studyTheory approach
5.0 Load estimation of wings
5.1 Force and moment calculation
5.2 Shear force diagram
5.3 Bending moment diagram
5.4
Spar location
6.0 Fuselage Design
6.1
Bulkhead design
6.2
Longeron calculation
6.3
Stringer calculation
7.0 Material Selection
8.0 3 D view of aircraft
9.0 Summary
10.0 References
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1. INTRODUCTION
The structural design of an airplane actually begins with the flight envelope or the
V-n diagram, which clearly limits the maximum load factors that the airplane can
withstand at any particular flight velocity. But, in normal practice the airplane might
experience loads that are much higher than the design loads. Some of the factors that lead
to structural overload of an airplane are high just velocities, sudden movement of the
controls, fatigue loads and in some cases, bird strikes or lightening strikes. So, to add
some inherent ability to withstand these rare but large loads, safety factor of 1.5 is
provided during the structural design.
The two major members than need to be considered for the structural design of an
airplane are the wings and the fuselage. As for as the wing design is concerned, the most
significant load is the bending load. So, the primary load bearing component in the wing
structure is the spar (the front and the rear spars) whose cross section is an I- section.
Apart from the spar to take the bending loads, suitable stringers need to be provided to
take shear loads acting on the wing.
Unlike the wing, which is subjected mainly to unsymmetrical bending load, thefuselage is much simpler for structural analysis due to its symmetrical cross section as
well as symmetrical loading. The main load in case of fuselage is only shear because the
load acting on the wing is transferred to the fuselage skin in the form of shear only. The
structural design of both the wing and the fuselage begin with shear force and bending
moment diagrams for the respective members. The maximum bending stress produced in
each of them is checked to be less than yield stress of the material chosen for the
respective member.
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1.1 THREE VIEW DIAGRAM FROM ADPI
FINAL SCALED PRELIMINARY DESIGN
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1.2IMPORTANT DATA FROM ADP1
AIRCRAFT INITIAL CONSIDERATIONS:
Mach 1.87(max)
Range 3200km
Cruise mach 1.14
Cruise altitude 16500m
W payload 5545kg
W take-off 23500 kg
Power plants F-135 P&W afterburning turbofan
AIRFOIL SELECTION:
NACA 64(3)-618 AIRFOIL
Thickness: 17.9%
Camber: 3.4%
Trailing edge angle: 12.4
o
Lower flatness: 35.9%
Leading edge radius: 2.4%
Max CL: 1.536
Max CLangle: 15.0
Max L/D: 38.202
Max L/D angle: 7.0
Max L/D CL: 1.331
Stall angle: -0.5
Zero-lift angle: -4.5
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Lift for NACA 64(3)-618 AIRFOIL
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2. V-n DIAGRAM
2.1 Introduction
The V-n diagram plays an important role in Aircraft design. The V-n diagram is a plot
between the load factor and the velocity. Load factor is defined as the ratio of the
aerodynamic load to the weight of the aircraft. Aircraft has to perform different loading
conditions at different speeds, controls and high loads due to stormy weather. But at the
same time, it is impossible to investigate all possible loading conditions. There are
structural limitations on the maximum load factor allowed for a given airplane. There are
two categories of structural limitations in airplane design:
1. Limit L oad Factor
This is the boundary associated with permanent structural deformation of one or more
parts of the airplane. If n is less than the limit load factor, the structure may deflect during
maneuver, but it will return to its original state when n = 1. If n is greater than the limit
load factor, then the airplane structure will experience a permanent deformation, i.e., it
will incurstructural damage.
2. Ul timate Load Factor
This is the boundary associated with outright structural failure. If n is greater than the
ultimate load factor, parts of the airplane willbreak.There arefour main critical conditions:
High Angle of Attack (+)
Low Angle of Attack (+)
Low Angle of Attack (-)
High Angle of Attack (-)
For airplane design, the limit load factor depends on the type of the aircraft.
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A typical V-n diagram looks like this:
2.2 Calculation of v-n diagram :
2.2.1 Takeoff, cruise and landing:
For positive curve,
From CLvs graph,
CL=1.56 and = 14
CL=0 and = -2
Lift slope for airfoil,a0= dCL / d
= 1.560 / 14(- 2)
a0=0.0975
Lift slope for wing, a = a0 / 1 + (64.72 a0/ e AR)
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= 0.0975 / 1+ (64.72(0.0975) / (0.8)(3.72))
a = 0.0658
co-efficient of lift , CL= a ( CLmax - CL = 0)
= 0.0658 ( 14( - 2 ) )
CL= 1.052
n = L/W = 1\2( V2S CL) / W
n = 1.624310-3V2
similarly for negative curve,
From CLvs graph,
CL= - 0.1 and = - 6
CL= - 0.4 and = -12
Lift slope for airfoil,a0= dCL / d
a0= 0.025
Lift slope for wing, a = a0 / 1 + (64.72 a0/ e AR)
a = 0.021311
co-efficient of lift , CL= a ( CLmax - CL = 0)
CL= - 0.1278
n = L/W = 1\2( V2S CL) / W
n = - 2.0290410-4
V2
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-5
-4
-3
-2
-1
0
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
0 25 50 75 100 125 150 175 200 225 250 275 300 325 350 375 400 425 450
Load
Factorn
Velocity (m)
V-n Diagram
vA
V
A'
Vc VD
Vc'
VD'
Stall area
Stall
area
Flight velocity (V) (m/s) npositive nnegative
0 0 0
10 0.162 0.09
20 0.64 0.36
30 1.46 0.81
40 4.06 1.44
50 6.80 2.25
64.72 7.95 3.03
388.88 9 3.03
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3.GUST ENVELOPE
TO FIND GUST LOAD FACTOR:
Gust loads are unsteady aerodynamic loads that are produced by atmospheric
turbulence. They represent a load factor that is added to the aerodynamic loads.
The effect of turbulence is to produce a short time change in the effective angle of
attack. This change can be either positive or negative, thereby producing an increase or
decrease in the wing lift and change in the load factor,=
.
The incremental load factor is then (from Design of aircraft by
Thomas.C.Corke,n =
u V CL2 W
S
(i)
Where,
n- Change in the load factor, -density at sea level (1.2256 kg/m3),u- Gust velocity
(m/s)V- Flight velocity (m/s), CL co efficient of lift, at max = 141.56 at ( =
0) =0.4,
Then,
npeak =nlevel flight+ n.. (ii)
The gusts that result from atmospheric turbulence occur in a fairly large band of
frequencies. Therefore, their effect on an aircraft depends on factors that affect its
frequency response. In particular, the frequency response is governed by an equivalent
mass ratio, ,defined as (from Design of aircraft by Thomas.C.Corke,
=
2WS
g c CL
Where,
-density at sea level (1.2256 kg/m3),
C L max = 1.56 (at flap deflection =14),
C L max = 0.4 (at flap deflection =0),
c- Average cord from wing design (12.815 m)
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the mass ratio , is a parameter in a response coefficient, K, which is defined differently
for supersonic,
K=1.03
6.95+1.03
The normal component of gust velocity, u, is the product of the normal average of values
taken from flight data, (u), and the response coefficient is (from Design of aircraft by
Thomas.C.Corke,
u=K u
GUST VELOCITY
At altitude of below 20000 ft the gust velocity is (from Design of aircraft by
Thomas.C.Corke,
Flight condition Altitude (m)Gust velocity ()
(m/)
K u (m/s)
High angle of
attack
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LOAD FACTOR
Gust envelop is,
-8
-7
-6-5
-4
-3
-2
-1
0
1
2
3
4
5
67
8
9
10
11
12
13
14
15
0 25 50 75 100 125 150 175 200 225 250 275 300 325 350 375 400 425 450
Load
Factorn
Velocity m
Gust EnvelopeVg
Vcruise
Vdive
Vg'V
cruise
'Vdive'
Dive condition 415.707 2.668628 11.66863
Flight condition Flight velocity (v) (m/), -
High angle of attack 112.09 1.07398 4.07398
Level flight 388.88 0.47341 3.47341
Dive condition 415.707 0.21677 3.21677
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The final V-n diagram is a combination of gust loads, maneuvering load factors
with the ultimate load factor. The ultimate load factor of any fighter aircraft is given by
multiplying the limit load factor with factor of safety. The final V-n diagram which
shows the possible operating region, limit load factor, ultimate load factor is shown
below the plot.
-8-7-6-5-4-3-2-101234
56789
10111213141516
0 25 50 75 100 125 150 175 200 225 250 275 300 325 350 375 400 425 450
Load
Fa
ctorn
Velocity m
Gust Envelope
vA
VA'
Vc VD
V
c'
VD'
Stall area
Stall areaVg'
Vg
Vcruise
Vdive
Vcruise'Vdive'
Flight velocity (V) (m/), Load factor (n) Load factor (n)
0 1 1
112.09 - 4.073
194.16 13.645 -
388.88 14.81 3.47
415.7 11.66 3.21
415.7 0 0
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Pulldown Maneuver
The pulldown maneuver is the inverted form of the pullup maneuver.
In this case, both lift and weight are contributing to the pitch rate - as a result, simply
rolling an airplane inverted will initiate this maneuver.
By convention, we will still consider lift and thus load factor positive as sketched.
Since the lift and weight are now in the same direction, the downward acting centripetal
forces is:
F =L +W =W(n +1) r
And the flight path radius of curvature and pitch down rate are given by:
=
2
=
2
(+1) =
=
(+1)
Note that as long as n > -1, R and are positive - for n=-1 the plane is in level flight;
for n < -1 the plane begins climbing in a pushup maneuver.
CACULATION OF PULL-UP AND PULL-DOWN V-n DIAGRAM
PULL-UP
The turn radius is given by: =
2
(1)
For the corner speed =64.72 m/s and limit loar factor n=10
=64.722
9.81(101)
R=53.37 m
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V in m n R
30 1.46187 198.8368
35 1.989768 126.2923
40 2.59888 102.1123
45 3.289208 90.26384
50 4.06075 83.34625
55 4.913508 78.87387
60 5.84748 75.78101
PULL-DOWN:
The turn radius is given by: =
2
(+1)
For the corner speed =64.72 m/s and limit loar factor n=10
=64.722
9.81(10+1)
R= 42.69m
V in m n R
30 1.46187 37.30365
35 1.989768 41.80927
40 2.59888 45.36559
45 3.289208 48.17502
50 4.06075 50.40795
55 4.913508 52.19803
60 5.84748 53.64703
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4. Structural design studyTheory approach
The structural design study of any aircraft includes the following
Wing design
The wing design and calculation of the lift distribution.
Drawing the bending moment and shear flow diagram.
Design of spars.
Fuselage design
Design of bulk heads.
Design of longerons.
Structural design criteria
The structural criteria define the types of maneuvers, speed, useful loads, and
gross weights which are to be considered for structural design analysis. These are items
which are under the control of the airplane operator. In addition, the structural criteria
must consider such items as inadvertent maneuvers, effects of turbulent air, and severity
of ground contact during landing. The basic structural design criteria, from which the
loadings are determined, are based largely on the type of the airplane and its intended
use.
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5. Load estimation of wings
Lift distribution over a delta wing
Lift distribution in a delta wing is a complex phenomenon involving vortex lift
and lift due to flow over the wing. In supersonic flow elliptic wing does not perform
optimally due to shock waves. So delta wings are used and so lift produced are in
accordance with the planform type, hence lift distribution in delta wing is linear without
vortex , but with vortex, lift becomes non-linear.
Lift distribution analysis
For our analysis ,the lift produced is assumed to be linear, this is reasonable for
analysis because vortex lift is upto 20% of total lift.
This can be given approximately by;
L(x)clc(y)
Where, x along span
y along chord
LINEAR LIFT DISTRIBUTION
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SHEAR FORCE AND BENDING MOMENT ANALYSIS OF WING
The more difficult loading is the linear distribution loading due to the lift on the
wing. The shear force distribution on the wing can be calculated by integrating the
loading function, the lift distribution, from the left free end to any point, x, on the wing,
The integration constant, C1, can be determined by using the boundary condition
that the shear force on the wing tip (x = -b) must be zero.
The calculated shear force values are,
X with Respect to
Wing rootShear force (KN)
1.8 108.4689
3.6 86.29647
4.95 71.329
5.4 66.65639
6.3 57.78599
7.2 49.54869
8.1 41.94449
9 34.97
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The shear force graph is plotted as,
Bending-Moments
The bending-moment is the force at each location on the spar that bends the wing
upward during normal non-inverted flight. The bending-moment is zero at the wing-tip
and maximum at the root. But its value is not proportional across the span. In other
words, it is not half as much at the wing mid-point as it is at the root. In fact, the mid-
point bending-moment is only about a 1/4 of the root value.
Thus, Similarly, the bending moment can be found by integrating the shear force
distribution, as
The bending moment force on the wing tip must be zero which is used to
determine the integration constant. The moment function become
0
20
40
60
80
100
120
140
-10 -5 0 5 10
Shear Force Diagram For Delta Wing
Wing Span m
SF ( KN)
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The calculated bending moment values are,
X with Respect to
Wing rootBending moment
(Nm)
1 563.3
2 426.24
3 287.46
4 62.35
5 26.75
6 12.68
7 4.68
8 0.327
The bending moment graph is plotted as,
0
100
200
300
400
500
600
700
-10 -5 0 5 10
Bending Moment Diagram for Delta
wing
BM (Nm)
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6. FUSELAGE DESIGN
Theory
The fuselage includes the cabin and/or cockpit, which contains seats for the occupants
and the controls for the airplane. In addition, the fuselage may also provide room for
cargo and attachment points for the other major airplane components. Some aircraft
utilize an open truss structure. The truss-type fuselage is constructed of steel or aluminum
tubing. Strength and rigidity is achieved by welding the tubing together into a series of
triangular shapes, called trusses.
Construction of the Warren truss features longerons, as well as diagonal and
vertical web members. To reduce weight, small airplanes generally utilize aluminum
alloy tubing, which may be riveted or bolted into one piece with cross-bracing members.
As technology progressed, aircraft designers began to enclose the truss members to
streamline the airplane and improve performance. This was originally accomplished with
cloth fabric, which eventually gave way to lightweight metals such as aluminum. In some
cases, the outside skin can support all or a major portion of the flight loads. Most modern
aircraft use a form of this stressed skin structure known as monocoque or
semimonocoque construction.
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The monocoque design uses stressed skin to support almost all imposed loads.
This structure can be very strong but cannot tolerate dents or deformation of the surface.
This characteristic is easily demonstrated by a thin aluminum beverage can. You can
exert considerable force to the ends of the can without causing any damage.
Partially Completed Structural Layout
Since no bracing members are present, the skin must be strong enough to keep the
fuselage rigid. Thus, a significant problem involved in monocoque construction is
maintaining enough strength while keeping the weight within allowable limits. Due to the
limitations of the monocoque design, a semi-monocoque structure is used on many of
todays aircraft.
The semi-monocoque system uses a substructure to which the airplanes skin is attached.
The substructure, which consists of bulkheads and/or formers of various sizes and
stringers, reinforces the stressed skin by taking some of the bending stress from the
fuselage.
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BULKHEADS
Any major vertical structural member of a semimonocoque fuselage, hull, or
float may be considered a bulkhead. Bulkheads serve to maintain the required external
contour at the station.Rib repair by patching. Where they are located. They also
give rigidity and strength to the structure. Bulkhead construction is similar to that used
for wing ribs. It consists of a web reinforced by angle stiffeners. The web is attached
to the skin by formed flanges or extruded angles, which serve as cap strips. Non-
watertight bulkheads may have lightening holes, and most bulkheads are cut out to
give clearance for stringers. The stringers are usually attached to the bulkhead by angle
clips. For our fighter,
The forward fuselage is 5.2m long and 1.7m wide.
The canopy is about 356 cm long and 114 cm wide.
The mid fuselage in 5.2 m long and 2m wide.
The aft fuselage is 5.8m long and 3.6m wide.
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LONGERONS
Most aircraft fuselages are constructed in sections and are of the
semimonocoque design. A longeron is a fore-and-aft member of the fuselage or nacelle
and is usually continuous across a number of points of support, such as frames and
bulkheads. The longerons, along with the stringers, are the major load-carrying members
and stiffeners.
The cross section we have chosen is I section, the no of longerons is given as
[(Max dia of fuselage)/spacings of longerons] = no of longerons
For our fighter,
Max dia =2 m
Spacing of longerons (referred to Jon Roskam) = 10 inch (.254m)
[2/.254]=7.87
Hence No. of longerons =8 (app).
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7. WING DESIGN
Wings develop the major portion of the lift of a heavier-than-air aircraft.Wing
structures carry some of the heavier loads found in the aircraft structure. The particular
design of a wing depends on many factors, such as the size, weight, speed, rate of climb,
and use of the aircraft. The wing must be constructed so that it holds its aerodynamics
shape under the extreme stresses of combat maneuvers or wing loading. Wing
construction is similar in most modern aircraft. In its simplest form, the wing is a
framework made up of spars and ribs and covered with metal. The construction of an
aircraft wing is shown in fig.Spars are the main structural members of the wing. They
extend from the fuselage to the tip of the wing. All the load carried by the wing is taken
up by the spars. The spars are designed to have great bending strength. Ribs give the
wing section its shape, and they transmit the air load from the wing covering to the spars.
Ribs extend from the leading edge to the trailing edge of the wing. In addition to the main
spars, some wings have a false spar to support the ailerons and flaps. Most aircraft wings
have a removable tip, which streamlines the outer end of the wing. Most Navy aircraft are
designed with a wing referred to as a wet wing. This term describes the wing that is
constructed so it can be used as a fuel cell. The wet wing is sealed with a fuel-resistant
compound as it is built. The wing holds fuel without the usual rubber cells or tanks. The
wings of most naval aircraft are of all metal, full cantilever construction. Often, they maybe folded for carrier use. A full cantilever wing structure is very strong. The wing can be
fastened to the fuselage without the use of external bracing, such as wires or struts. A
complete wing assembly consists of the surface providing lift for the support of the
aircraft. It also provides the necessary flight control surfaces.
Strength of Wings
Uniformly built spars, having the same structure and dimensions from the root to
even just halfway to the wing-tip, add weight with little benefit in strength, and thisweight is closer to the wing-tips which inhibit rolls in both fighter planes, as well as
sailplanes. While spar design may be an interesting engineering challenge. Uniformly
built spars are simple to construct.
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Maximum Wing-Load
First let's make it clear that maximum wing-load is not the same as wing-loading.
The maximum wing-load is the force when the plane is performing a maximum-G
manoeuvre. Fighter planes may experience maximum-G during a high speed turn, or pull-
up from a high speed dive. Figure shows the load forces in banked turns.
Figure G-load vs Bank Angle
Figure-7.3 shows the maximum load forces at the bottom of a verticle loop. At the top of
the loop, gravity is aiding the plane in pulling toward the center of the loop, while at the
bottom, it is pulling it out of the loop. The figure shows how the loads increase with
speed, and with smaller diameter loops. Even if the plane is not being flown in a
complete loop, these numbers still apply if the plane is simply being pulled out of a dive.
G-load in verticle loops
The point is that the maximum load is far greater than simply the weight of the plane.
Three things need to be considered:
The weight of the plane less the weight of the wings, W sub b.
The maximum-Gs the plane experiences in flight, N.
A safety-factor accounting for material and construction flaws, S.
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The wings are assumed to support themselves, therefore, the wing root only supports
the weight of the fuselage and tail. However, this weight may be multiplied many times
determined by the maximum-Gs experienced during a flight maneuver. The value of N
would be 3, if a 3G flight maneuever is the worst case. This would result in a maximum
of N* W b.
Bending Strength
Knowing the bending-moment across the span determines the required bending-
strength of the spar. The bending-strength is determined by the structure of the spar, its
shape, and the materials used. In the same way that the bending-moment of the wing was
not as simple as our simple approximation for a rectangular wing, determining the
equations for the bending-strength of the spar is also not simple and straight-forward. The
problem is that the force is linearly varying from zero at the neutral-axis to its maximum
at the surface. However, the equations are well known for I-beam and comparable
structures. The bdimension represents the total empty space within the beam and may be
split, as in the case of an I-beam.
Figure 7.5 - Spar Structure
B H3- b h
3
M = -----------
6 H
Figure-7.6 compares the accurate moment-of-inertia calculation to several
approximations. The approximations are based on the cross-sectional area of the spar-
cap, A = b Tc. Each approximation multiplies the area, A, by: 1) the full spar-height, H,2) the distance between the midpoints of both spar caps, (H-h)/2, and 3) the distance
between the spar-caps, h = H-2Tc. The curves illustrate how all approximations become
increasingly accurate as the spar-caps become thinner.
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Figure 7.6 - Comparision of Moment-of-Inertia calculation and approximations vs spar-
cap thickness (1" spar)
Only the last approximation, using the distance between the spar-caps, is
conservative in that it errors on the side of under estimating the strength. It is also
relatively accurate. This approximation has less than 5% error for the case where the
spar-caps are less-than 15% of the spar thickness. This is certainly the case for 1/8" spar-
caps in a 7/8" spar, more typical in wooden construction. High-performance structures
using thin (~3%) carbon-fiber laminates can use the most convenient approximation
accurately.
Shear-Strength
The forces involved in resisting the bending-moment of the wing are parallel to
the spar. The spar must also support the weight of the plane as it is distributed across thewing. Like the previous calculations, it must consider the lift distribution across the wing.
A simple conservative approximation assumes a proportionally decreasing load from the
maximum load at the root, to zero load at the wing-tip. Figure-6 shows actual values for
several planforms. It shows that for an elliptical planform, the shear is actually 40% of
the max at the midpoint of the halfspan.
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Spar definition
The maximum bending moment from previous section was found to be as
583035.21 Nm. Therefore we define 3 Spars with front spar at 15% of chord, middle spar
at 45% of chord and rear spar at 70% of chord. The position of the three spars from the
leading edge of the root chord is given below as follows
Possible Spar Location
Front spar - 15% of chord = 2.25 m
Middle spar - 45% of chord = 6.75 m
Rear spar - 70% of chord = 10.5 m
Bending moment M = Max BM * FOS * n
= 583035.21 1.5 8.932
= 7811851.79Nm
The Structural load bearing members in the wing are the Spars and Stringers. Thebending moment carried by the Spars is 70% and that of Stringers is 30% of the total
Bending Moment.
Bending Moment taken by Spars is = 0.7 x 7811851.79Nm = 5468296.25 Nm
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WING CONSTRUCTION:
1. WING FUEL TANKS
In addition to providing the required strength and stiffness, the structural
box almost always has to provide fuel space. Integral tanks, as opposed to separate
internally supported types, are preferred since their use enables the maximum advantage
to be taken of the available volume. Integrally machined or molded constructions, which
use a small amount of large components, are obviously an advantage since sealing is
reduced to a minimum. The major problem occurs at tank end ribs, particularly in the
corners of the spar web and skins, and at lower surface access panels. The corner
difficulty is overcome by using special suitcase corner fittings.
Access panels should be large enough for a person to get through so that
the inside can be inspected and resealed if necessary. On shallow section wings, the
access has to be in the lower surface so that the operator can work in an acceptable way
even if the depth is insufficient to climb in completely. Apart from the sealing problems,
lower surface access panels are in what is primarily a tension skin and so introduce stress
concentrations in an area where crack propagation is a major consideration. The access
panels are arranged in a span-wise line so the edge reinforcing can be continuous andminimum stress concentration due to the cut-outs. Access panels are often designed to
carry only shear and pressure loads, the wing bending being reacted by the edge
reinforcing members. A deep wing can avoid these problems by using upper surface
access panels but this is not a preferred aerodynamic solution.
2. RIB LOCATION AND DIRECTION
The span-wise location of ribs is of some consequence. Ideally, the rib
spacing should be determined to ensure adequate overall buckling support to the
distributed flanges. This requirement may be considered to give a maximum pitch of the
ribs. In practice other considerations are likely to determine the actual rib locations such
as:
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a) Hinge positions for control surfaces and attachment/operating points for flaps,
slats, and spoilers.
b) Attachment locations of power plants, stores and landing gear structure.
c) A need to prevent or postpone skin local shear or compression buckling, as
opposed to overall buckling. This is especially true in a mass boom form of
construction.
d) Ends of integral fuel tanks where a closing rib is required. When the wing is
sweep back, it is usual for the ribs to be arranged in the flight direction and
thereby define the aerofoil section. While the unswept wing does give
torsional stiffness, the ribs are heavier, connections are more complex and in
general the disadvantages overweigh the gains.
3. HORIZONTAL STABILISER
When the horizontal stabilizer is constructed as a single component across the
centerline of the aircraft, the basic structural requirements are very similar to those of a
wing.
4. VERTICAL STABILISER
The vertical stabilizer presents a set of issues which are different from those of the
main plane or horizontal stabilizer. Relevant matters are:
a) It is not unusual to build the vertical stabilizer integrally with the rear fuselage.
The spars are extended to form fuselage frames or bulkheads. A root rib is
made to coincide with the upper surface of the fuselage and is used to transmit
the fin root skin shears directly into the fuselage skin. Fin span-wise bending
results in fuselage torsion. Often it is logical to incline the rear spar bulkhead to
continue the line of the rear spar since it is usually the end of the main fuselage
structure. On the other hand, the front spar and any intermediate attachment
frames are often best kept perpendicular to fuselage fore and aft datum. The
change in direction being made at the fin root rib. Otherwise the structural form
can follow that of a wing.
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b) Sometimes on smaller aircraft the fin is designed as a separate component which
may readily be detached. The fin attachment lugs are arranged in both lateral and
fore and aft directions so that in addition to vertical loads they react side and drag
loads.
HIGH LIFT SYSTEMS:
There is a wide variety of leading and trailing edge high-lift systems. Some
types are simply hinged to the wing, but many require some degree of chord-wise
extension. This can be achieved by utilizing a linkage, a mechanism, a pivot located
outside the aerofoil contour or, perhaps most commonly, by some from of track. Trailing
edge flaps may consist of two or more separate chord-wise segments, or slats, to give a
slotted surface and these often move on tracts attached to the main wing structure.
The majority of flaps and slats are split into span wise segments of no greater
lengths than can be supported at two or three locations. As with control surfaces, the
locations of the support points are established so as to minimize local deformations since
the various slots are critical in determining the aerodynamic performance. Sometimes the
actuation may be located at a different pan wise position from the support points. This is
often a matter of convenience, layout clearances, and the like.
The structural design of flaps is similar to that of control surfaces but its simpler
as there is no requirement for mass balance, the operating mechanisms normally being
irreversible. On large trailing edge flap components, there is often more than one spar
member. Especially when this assists in reacting the support or operating loading. There
may be a bending stiffness problem in the case of relatively small chord slat segments
and full depth honey combs can be used to deal with this. Figure shows a cross section of
a typical slotted flap of metal construction but the same layout applies if composite
materials are used.
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Delta Wings:
A delta wing is awing whose shape when viewed from above looks like a
triangle, often with its tip cut off. It sweeps sharply back from the fuselage with the angle
between the leading edge (the front) of the wing often as high as 60 degrees and the angle
between the fuselage and the trailing edge of the wing at around 90 degrees. Often delta-
wing airplanes lack horizontal stabilizers. Despite the fact that paper airplanes have delta
wings and appear to fly quite well when launched from a height, delta wings actually
perform poorly at low speeds and often are unstable (i.e., they do not stay in level flight
on their own). Their primary advantage is efficiency in high-speed flight.
By 1953, Convair's engineers had developed the YF-102 Delta Dagger, a radical
design that lacked a horizontal tail and featured a large, sharply swept delta wing. Wind
tunnel tests of small-scale models indicated that the aircraft could accelerate through
Mach 1 (the speed of sound) with relative ease, rather than "punching" through it like
earlier experimental planes that had to burn a lot of fuel to go faster than Mach 1.
However, the first prototype unexpectedly encountered immense drag as it approached
Mach 1. This so-called "transonic" region presented a major problem for the aircraft.
Near the same time, Richard T. Whitcomb, an aeronautical scientist at
theNational Advisory Committee for Aeronautics (NACA), was studying transonic drag.
Whitcomb developed what he called the "supersonic area rule." This theory stated that
aircraft that would fly at supersonic speed should increase in cross-sectional area from a
pointed nose. Anything that protruded into the airstream, such as the canopy over the
cockpit, wings, or tail, should be accompanied by a reduction in cross-section elsewhere.
In 1954, Whitcomb, who was then only 33-years old, was awarded the prestigiousCollier
Trophy for this contribution to aeronautics.
Convair's designers quickly applied the supersonic area rule to a new aircraft, the
YF-102A, pinching the fuselage near its mid-point to give it a slightly hourglass (or
Coke-bottle) appearance. This was a compromise for an existing aircraft; later airplanes
included the area rule in their designs in much less obvious ways. When the first YF-
102A with this new design took flight, it easily accelerated through Mach 1.
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The two most famous current aircraft to use the delta wing are theConcorde and
the Space Shuttle. The Concorde's delta wing made the plane's sustained cruising speed
of Mach 2 possible. The Space Shuttle's wing, known as a "cranked delta" because the
leading edge of the wing has a slight bend near its midpoint, is used for a different
purpose. The Space Shuttle originally had what was known as a "high crossrange"
requirement, which was the ability to glide for thousands of miles to either side of its
flight path when landing. Conventional straight wings did not provide enough lift at high
speeds and altitudes to achieve this type of range, and so the large delta wing was
necessary.
While delta wings are critical to achieving high lift for supersonic flight, they also
have a number of disadvantages for less high-performing aircraft. They require high
landing and takeoff speeds and long takeoff and landing runs, are unstable at high angles
of attack, and produce tremendous drag when "trimmed" to keep the plane level. Of these
disadvantages, pilots and designers usually consider the high landing and takeoff speeds
the most important because they make flying the plane dangerous. Indeed, when the
Concorde had its first ever crash in 2000, after two decades of safe operations, the high-
speed takeoff was a factor in this terrible accident, for the plane's high ground speed
before becoming airborne placed major stress upon the aircraft's tires, which exploded
upon striking an object on the runway.
Computer-controlled "fly-by-wire" flight control systems have allowed designers
to compensate for some of the delta wing's poor control qualities. Canards are small
horizontal fins (or small wings) mounted on the fuselage in front of an aircraft's main
wings to provide greater control, particularly during high angles of attack. When they are
part of a delta-wing aircraft, they improve its stability and maneuverability.
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8. MATERIALS
8.1 Materials used in aircraft manufacturing:
For many years, aircraft designers could propose theoretical designs that they
could not build because the materials needed to construct them did not exist. (The term
"unobtainium" is sometimes used to identify materials that are desired but not yet
available.)
The techniques for building aircraft evolved gradually during the years between
the wars. Wood and canvas changed to aluminum as the principal structural material
while designs improved and records were set and broken. Monoplanes (single wing
aircraft) were becoming more popular than biplanes (two wing aircraft).
Material requirement for aircraft building:
small weight
high specific strength
heat resistance
fatigue load resistance
crack and corrosion resistance
8.2 Titanium alloy
Titanium alloysaremetallicmaterials which contain a mixture oftitanium and
otherchemical elements.Such alloys have very hightensile strength andtoughness (even
at extreme temperatures), light weight, extraordinary corrosion resistance, and ability to
withstand extreme temperatures. However, the high cost of both raw materials and
processing limit their use tomilitary applications,aircraft, spacecraft, medical
devices,connecting rods on expensivesports cars and some premiumsports
equipment andconsumer electronics. Auto manufacturers Porsche and Ferrari also use
titanium alloys in engine components due to its durable properties in these high stress
engine environments.
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8.3 ALUMINIUM ALLOY:
Aluminium alloys arealloys in whichaluminium (Al) is the predominant metal.
The typical alloying elements arecopper,magnesium, manganese,silicon andzinc.There
are two principal classifications, namelycasting alloys and wrought alloys, both of which
are further subdivided into the categoriesheat-treatable and non-heat-treatable. About
85% of aluminium is used for wrought products, for example rolled plate, foils
andextrusions. Cast aluminium alloys yield cost effective products due to the low
melting point, although they generally have lowertensile strengths than wrought alloys.
The most important cast aluminium alloy system is Al-Si, where the high levels of silicon
(4.0% to 13%) contribute to give good casting characteristics. Aluminium alloys are
widely used in engineering structures and components where light weight or corrosion
resistance is required.
Wrought alloys:
The International Alloy Designation System is the most widely accepted naming scheme
forwrought alloys.Each alloy is given a four-digit number, where the first digit indicates
the major alloying elements.
1000 series are essentially pure aluminium with a minimum 99% aluminium content by
weight and can bework hardened.
2000 series are alloyed with copper, can beprecipitation hardened to strengths
comparable tosteel.
3000 series are alloyed with manganese, and can bework hardened.
4000 series are alloyed with silicon. They are also known assilumin.
5000 series are alloyed with magnesium.
6000 series are alloyed with magnesium and silicon, are easy to machine, and can be
precipitation hardened, but not to the high strengths that 2000 and 7000 can reach.
7000 series are alloyed withzinc, and can be precipitation hardened to the highest
strengths of any aluminium alloy.
8000 series is a category mainly used for lithiumalloys.
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Cast alloys:
The Aluminium Association (AA) has adopted a nomenclature similar to that of wrought
alloys.British Standard and DIN have different designations. In the AA system, the
second two digits reveal the minimum percentage of aluminium, e.g. 150.x corresponds
to a minimum of 99.50% aluminium. The digit after the decimal point takes a value of 0
or 1, denoting casting and ingot respectively. The main alloying elements in the AA
system are as follows:
1xx.x series are minimum 99% aluminium
2xx.x series copper
3xx.x series silicon, copper and/or magnesium
4xx.x series silicon
5xx.x series magnesium
7xx.x series zinc
8xx.x series lithium
Named alloys:
Alclad Aluminium sheet formed from high-purity aluminium surface layers bonded to
high strength aluminium alloy core material
Birmabright (aluminium, magnesium) a product of The Birmetals Company, basically
equivalent to 5251
Duralumin (copper, aluminium)
Magnalium
Magnox (magnesium, aluminium)
Silumin (aluminium, silicon)
Titanal (aluminium, zinc, magnesium, copper, zirconium) a product ofAustria Metall
AG.Commonly used in high performance sports products, particularly snowboards and
skis.
Y alloy,Hiduminium,R.R. alloys: pre-warnickel-aluminium alloys, used in
aerospace and engine pistons, for their ability to retain strength at elevated temperature.
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Applications
Aerospace alloys
Scandium-Aluminium
The main application of metallic scandium by weight is inaluminium-scandium
alloys for minor aerospace industry components. These alloys contain between 0.1% and
0.5% (by weight) of scandium. They were used in the Russian military aircraft Mig
21 andMig 29.
List of aerospace Aluminium alloys:
The following aluminium alloys are commonly used inaircraft and
otheraerospace structures:
7075 aluminium
6061 aluminium
6063 aluminium
2024 aluminium
5052 aluminium
8.4. Composites:
For many years, aircraft designers could propose theoretical designs that they
could not build because the materials needed to construct them did not exist. (The term
"unobtainium" is sometimes used to identify materials that are desired but not yet
available.) For instance, large space planes like the Space Shuttle would have proven
extremely difficult, if not impossible, to build without heat-resistant ceramic tiles to
protect them during re-entry.
Fiberglass is the most common composite material, and consists of glass fibers
embedded in a resin matrix. Fiberglass was first used widely in the 1950s for boats and
automobiles, and today most cars have fiberglass bumpers covering a steel frame.
Fiberglass was first used in the Boeing 707 passenger jet in the 1950s, where it comprised
about two percent of the structure.
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8.4.1 Carbon Fiber:
Carbon fibre is the reinforcement material of choice for "advanced" composites,
particularly following significant price reductions over the past decade. A major
advantage of carbon fibres is their higher fatigue resistance compared to glass orAramid.
Unlike these last two materials, carbon fibres do not suffer from stress rupture. Carbon
fibres are supplied in tows and may vary from 1000 fibres per tow to hundreds of
thousands of fibres per tow.
8.4.2 KEVLAR:
Kevlar is the registered trademark for a para-aramid synthetic fiber, related to
other aramids such as Nomex and Technora. Developed at DuPont in 1965, this high
strength material was first commercially used in the early 1970s as a replacement for
steel in racing tires. Typically it is spun into ropes or fabric sheets that can be used as
such or as an ingredient in composite material components.
8.4.3 FIBERGLASS:
Fiberglass, (also called fibreglass and glass fibre), is material made from
extremely fine fibers of glass. It is used as a reinforcing agent for many polymer
products; the resulting composite material, properly known as fiber-reinforced polymer
(FRP) or glass-reinforced plastic (GRP), is called "fiberglass" in popular usage.
Glassmakers throughout history have experimented with glass fibers, but mass
manufacture of fiberglass was only made possible with the invention of finer machine
tooling.
Just some applications for aerospace fiberglass:
Aircraft Enclosures for Controls
Antenna Enclosures
Storage Bins
Luggage Racks
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8.4.4 BORON FIBER:
Specialty Materials boron fiber is particularly desirable for use in aerospace
industry applications where high compression loads are present. Some examples of these
applications include the following aircraft: F-15 Fighter, F-14 Fighter, B1 Bomber,
Blackhawk Helicopter, Predator B UAV, and the Space Shuttle. Additionally, Specialty
Materials boron fiber has been used to repair aircraft structures in both military and
commercial aircraft including the B-52, C-130, F-4, F-5, F-111 and Boeing 727, 747, 757
and MD-11. Please see the chart below for reference.
Aircraft Manufacturer MaterialApplication
BoeingBoron/Epoxy
Horizontal
and vertical
tail skins
rudder
Grumman
AerospaceCorp.
Boron/Epoxy
Horizontal tail
skins
Rockwell
International Boron/Epoxy Dorsal Longeron
Sikorsky Boron/Epoxy Rotor Blades and
Stabilator
General AtomicsBoron/ Graphit e
Epoxy Top Beam Cap
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8.5. Radar-absorbent material
Theory
Radar-absorbent material, or RAM, is a class of materials used in stealth
technology to disguise a vehicle or structure from radar detection. A material's
absorbency at a given frequency of radar wave depends upon its composition. RAM
cannot perfectly absorb radar at any frequency, but any given composition does have
greater absorbency at some frequencies than others; there is no one RAM that is suited to
absorption of all radar frequencies. A common misunderstanding is that RAM makes an
object invisible to radar. A radar absorbent material can significantly reduce an object's
radar cross-section in specific radar frequencies, but it does not result in "invisibility" on
any frequency. Bad weather may contribute to deficiencies in stealth capability. A
particularly disastrous example occurred during the Kosovo war, in which moisture on
the surface of an F- 117 Nighthawk allowed long-wavelength radar to track and shoot it
down. RAM is only a part of achieving stealth.
Types of RAM
Iron ball paint
One of the most commonly known types of RAM is iron ball paint. It contains
tiny spheres coated with carbonyl iron or ferrite. Radar waves induce molecularoscillations from the alternating magnetic field in this paint, which leads to conversion of
the radar energy into heat. The heat is then transferred to the aircraft and dissipated. The
iron particles in the paint are obtained by decomposition of iron pentacarbonyl and may
contain traces of carbon, oxygen and nitrogen.
Foam absorber
Foam absorber is used as lining of anechoic chambers for electromagnetic
radiation measurements. This material typically consists of fireproofed urethane foam
loaded with carbon black, and cut into long pyramids. The length from base to tip of the
pyramid structure is chosen based on the lowest expected frequency and the amount of
absorption required. For low frequency damping, this distance is often 24 inches, while
high frequency panels are as short as 3-4 inches. Panels of RAM are installed with the
tips pointing inward to the chamber.
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Jaumann absorber
A Jaumann absorber or Jaumann layer is a radar absorbent device. When first
introduced in 1943, the Jaumann layer consisted of two equally-spaced reflective surfaces
and a conductive ground plane. One can think of it as a generalized, multilayered
Salisbury screen as the principles are similar.
More elaborate Jaumann absorbers use series of dielectric surfaces that separate
conductive sheets. The conductivity of those sheets increases with proximity to the
ground plane.
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9. 3D DIAGRAM
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9. Summary
V-n characteristics for positive load factor [n limpositive= 9]
VA(Design Maneuvering Speed) = 195.72 m/s.
VC(Design Cruising Speed) = 388.88 m/s.VD(Design Diving Speed) = VC + 26.82m/s =412.7m/s.
V-n characteristics for negative load factor [n limnegative= -3]
VS (Stalling speed) = 64.72m/s.
VA = 61.83=112.02 m/s.
VC (Cruise speed) = 388.88 m/s.
VD (Diving speed) = VC + 26.82m/s = 412.72m/s.
V-n characteristics for gust load
Maximum gust load factor = 8.439.
Minimum gust load factor = -3.2.
Load estimation of wings
Maximum shear force =108468.9N
Maximum bending moment=532378.9Nm.
Fuselage design
The forward fuselage is 5.2m long and 1.7m wide.
The canopy is about 356 cm long and 114 cm wide.
The mid fuselage in 5.2 m long and 2m wide.
The aft fuselage is 5.8m long and 3.6m wide.
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Materials used
Aluminium: Fuselage (because they are corrosion resistant and have high
strength to weight ratio.
Transparent Plastic: Transparent plastic is used in canopies, windshields, and
other transparent enclosures.
Kevlar: for racing tires.
Boron fiber: Particularly desirable for use in aerospace industry applications
where high compression loads are present.
Reinforced Plastic: Reinforced plastic is used in the construction of radomes,
wingtips, stabilizer tips, antenna covers, and flight controls. It has high strength-
to-weight ratio and is resistant to mildew and rot. Suitable for other parts of the
aircraft.
Design
Thus the final sketches of Aircraft design project II are made using the three view
diagram of our Aircraft design project I.
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10. REFERENCES
Raymer, D.P., Aircraft Design: A Conceptual Approach, Third Edition, AIAA,
Inc., Reston, VA, pp. 229-270, 379-401, 406, 408-412, 426-446, 2006.
Roskam, Jan., Airplane Design, Roskam Aviation and Engineering Corporation,
Ottawa, KS, 2007.
Raymer, D.P., Aircraft Design: A Conceptual Approach, Second Edition, AIAA,
Inc., Reston, 2006.
Lloyd R. Jenkinson and James F. Marchman III, Aircraft Design Projects forengineering students, 2003.
John D. Anderson, Aircraft Performance and Design, Tata McGraw-Hill Edition
2010.
John D. Anderson, Fundamentals of Aerodynamics, Tata McGrraw-Hill Edition
2010.
Airfoil Investigation Database,http://www.worldofkrauss.com/foils.
F136 Engine- Best Of Both Worlds, http://f136engine.com
Stability Performances and Analysis, Wing Loading Estimation
http://adamone.rchomepage.com
Composites
http://hsc.csu.edu.au/engineering_studies/aero_eng/2579/polymer_composites.ht
ml
V-n Diagramhttp://adg.stanford.edu/aa241/structures/ivn.html
Shear Force and Bending Moment Diagrams
http://www.transtutors.com/homework-help/Mechanical+Engineering/Bending+Moment+and+Shear+Force/cantilever-
subjected-to-uniformly-varying-load.aspx
http://adamone.rchomepage.com/http://adamone.rchomepage.com/http://hsc.csu.edu.au/engineering_studies/aero_eng/2579/polymer_composites.htmlhttp://hsc.csu.edu.au/engineering_studies/aero_eng/2579/polymer_composites.htmlhttp://hsc.csu.edu.au/engineering_studies/aero_eng/2579/polymer_composites.htmlhttp://adg.stanford.edu/aa241/structures/ivn.htmlhttp://adg.stanford.edu/aa241/structures/ivn.htmlhttp://www.transtutors.com/homework-help/Mechanical+Engineering/Bending+Moment+and+Shear+Force/cantilever-subjected-to-uniformly-varying-load.aspxhttp://www.transtutors.com/homework-help/Mechanical+Engineering/Bending+Moment+and+Shear+Force/cantilever-subjected-to-uniformly-varying-load.aspxhttp://www.transtutors.com/homework-help/Mechanical+Engineering/Bending+Moment+and+Shear+Force/cantilever-subjected-to-uniformly-varying-load.aspxhttp://www.transtutors.com/homework-help/Mechanical+Engineering/Bending+Moment+and+Shear+Force/cantilever-subjected-to-uniformly-varying-load.aspxhttp://www.transtutors.com/homework-help/Mechanical+Engineering/Bending+Moment+and+Shear+Force/cantilever-subjected-to-uniformly-varying-load.aspxhttp://www.transtutors.com/homework-help/Mechanical+Engineering/Bending+Moment+and+Shear+Force/cantilever-subjected-to-uniformly-varying-load.aspxhttp://www.transtutors.com/homework-help/Mechanical+Engineering/Bending+Moment+and+Shear+Force/cantilever-subjected-to-uniformly-varying-load.aspxhttp://adg.stanford.edu/aa241/structures/ivn.htmlhttp://hsc.csu.edu.au/engineering_studies/aero_eng/2579/polymer_composites.htmlhttp://hsc.csu.edu.au/engineering_studies/aero_eng/2579/polymer_composites.htmlhttp://adamone.rchomepage.com/