final 1200 (1)
TRANSCRIPT
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ABBREVIATION
- Density of air
- Dynamic viscosity
- Taper ratio
AR - Aspect ratio
b - Wing span
S - Wing area
Swet - Wetted area
Sref - Reference area
C - Chord of the airfoil
Croot - Chord at root
Ctip - Chord at tip
CD - Drag Co-efficient
CL - Lift Co-efficient
D - Drag
L - Lift
E - Endurance
g - Acceleration due to gravity
M - Mach number of aircraft
R - Range
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- Climb Angle
T - Thrust
Re - Reynolds number
ROC - Rate of climb
SL - Landing distance
STO - Take off distance
VCruise- Velocity at cruise
Vstall - Velocity at stall
WCrew - Crew weight
We - Empty weight of aircraft
WF - Weight of fuel
Wpayload- Payload of aircraft
W0 - Overall weight of aircraft
WL - Wing loading
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ABSTRACT
The purpose of our design project was to design a 200 seater passeng
medium range international aircraft by comparing the data and specifications
present aircrafts in this category. Performance characteristics calculations have al
been performed. Necessary graphs have also been plotted from where certa
values where deduced. The aircraft possess a low wing, tricycle landing gear andconventional tail arrangement.
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COMPARATIVE DATA SHEET
Sl no Name of a/c No of
seats
Service
ceiling (km)
Wing span
(m)
Wing area
(m2)
Aspect ratio
1 Bombardier crj100 50 12496 21.21 48.35 16:9
2 Bombardier crj200 50 12496 21.21 48.35 16:9
3 Antonov An-140 52 7600 24.505 51 16:9
4 Fokker-50 58 7620 29 70 12:1
5 Bombardier-Dash 8 50 7680 27.43 56.2 11:1
6 CASA/IPTN CN-235 44 7620 25.8 59.1 11.27:1
7 ATR-42 50 7600 24.5 54.5 11.1:1
8 XIAN MA600 60 7622 29.2 72 12:1
9 VISCOUNT V 700 60 7620 28.56 89 11:1
10 Saab 2000 58 9450 24.76 55.7 11:0
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Sl no Name of a/c Type of engine No of engine Thrust power (KW)
1 Bombardier crj100 2 Turbo prop 6830
2 Bombardier crj200 2 Turbo prop 6875
3 Antonov An-140 2 Turbo prop 1,838
4 Fokker-50 2 Turbo prop 1,864
5 Bombardier Dash 8
Q-300
2 Turbo prop 6875
6 CASA/IPTN CN-235 2 Turbo prop 1,305
7 ATR_42 2 Turbo prop 1465
8 Xian ma 600 2 Turbo prop 2148
9 Vickers viscount v700 2 Turbo prop 1484
10 Saab 2000 2 Turbo prop 3096
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s
Sl no Name of a/c Empty fuel wt (n) Maximum takeoffwt (kg)
Payload (n)
1 Bombardier crj100 13650 24041 6124
2 Bombardier crj200 13830 24041 6124
3 Antonov An-140 12810 21500 13227
4 Fokker-50 12250 20820 6080
5 Bombardier Dash 8
Q-300
19500 2720
6 CASA/IPTN CN-235 9800 15100 4000
7 ATR_42 10600 15550 4500
8 Xian ma 600 13700 21800 5500
9 Vickers viscount v700 16718 30617 6000
10 Saab 2000 13800 22800 5900
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Sl no Name of a/c Range (km) Cruise Speed
(km/hr)
Wing
loading
MAXIMUM
TAKE OFF
SPEED
1 Bombardier crj100 3000 860 497.22 786
2 Bombardier crj200 3045 860 497.22 786
3 Antonov An-140 3270 540 421.23 540
4 Fokker-50 2055 560 297.4
5 Bombardier Dash 8
Q-300
2055 500 346.97
6 CASA/IPTN CN-235 4355 450 255.49
7 ATR_42 1950 500 285.32
8 Xian ma 600 2450 514 302.77
9 Vickers viscount v700 2600 522 344.01
10 Saab 2000 2100 685 409.33
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0
2000
4000
6000
8000
10000
12000
14000
0 1000 2000 3000 4000 5000
Serviceceiling(km)
Range (km)
Service ceiling (km)
Service ceiling (km)
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0
100
200
300
400
500
600
0 1000 2000 3000 4000 5000
Wingloading
Range(km)
Wing loading VS Range
Wing loading
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0
100
200
300
400
500
600
700
800
900
1000
0 1000 2000 3000 4000 5000
CruiseSpeed(km/hr)
Range(km)
Cruise Speed (km/hr)
Cruise Speed (km/hr)
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10:55
11:02
11:09
11:16
11:24
11:31
11:38
11:45
11:52
12:00
12:07
0 500 1000 1500 2000 2500 3000
Aspectratio
Range (km)
Aspect ratio
Aspect ratio 16:09 16:09 16:09
12:01 11:01 11.27:1 11.1:1
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0
50
100
150
200
250
300
350
400
0 1000 2000 3000 4000 5000
THRUSTTOWEIGHT
RANGE
RANGE VS THRUST TO WEIGHT RATIO
Series1
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SL.NO SPICIFICATION DATA
1. Aspect ratio10.9
2. Cruise speed 520KM\Hr
3. Service ceiling 7800M
4. Thrust to weightratio
110
5. Range 2500KM
6. Wing loading 320
7. Max takeoff weight 21000KG
8. L/D ratio 12.2
9. Max takeoff speed
10. Endurance 6.51hrs
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OVERALL WEIGHT ESTIMATION:
The structural design , the complexity of the load distributio
through a redundant structure , and the large number of sophisticate
systems in an a/c , makes weight est a difficult and precarious task.
When the detail design drawing are complicit, the engg s cal the wt
each and every part, and add all and cal the wt. But in the beginnin
phase of design process, this cannot be accomplished because there a
neither detailed drawing of the a/c nor the detail of the various parts the a/c.
And so some approximations are made and overall weight is eventually
estimated.
Overall takeoff weight is given by,
W crew + w payload
W0= .
[1-(we/w0)-(wf/w0)]
Where:-
Wc =crew wt
Wp =payload wt
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Wf =fuel wtWe =structural wt
First approximation:
WC+wp.1
(w0)1 =
[1-(we/WO)-(wf/w0)]
Where:-
(We/w0)= [(Wfixed/w0)+(Wpower plant/w0)+(wstructural/w0)]
Given:
W structural=0.3wo
W power plant=0.06wo
W fixed equipment=0.045wo
W fuel=0.15wo
(We/w0) =0.045+0.06+0.3=0.405
(Wf/w0) =0.15
(WC+wp.1) =1000N+700N=1700N (for one passenger)
*In this we have forty persons including the pilot so,
[Wc/wp.1]=50*1700=85000N
(w0)1= 85000
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= 191011.236N
[1-0.405-0.15]
Second approximation:
Now from the graph of (we/w0) and the max takeoff wt,
We get,
According to a/c max takeoff wt Is 15000kg and (we/w0) =0.405
We know for complete one flight we can separate as
Warm up and take off
Climb
Cruise
Loiter
Desent Landing
[(wf/w0)=1.06(1-(wx/w0)]
Where,
(Wx/w0) = (w1/wo)(w2/w1)(w3/w2)(w4/w3)(w5/w4)(w6/w5)
General flight pattern of forty seated aircraft:
WHERE:-
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(W1/wo) =warm up and takeoff
(W2/w1) = climb
(W3/w2)= cruise
(W4/w3)= loiter
(W5/w4)= Desent
(W6/w5)= landing
(W1/wo)= (wi/wi-1) =0.96
(W2/w1)=0.98
(W3/w2) = (wi/wi-1) +exp^ (-RC/V (L/D))
Where
R=range=2400km
V=max takeoff speed=520km/hr
C=Sp fuel consumption
For TURBOPROP type of engine which we have to select &value from
the table
Cbhp =0.6 and p =0.8
So,
C=0.6*520/550*0.8= 0.78
(W3/W2)=e^(-(2400*0.78/520*14.2))=0.77
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(W4/W3)=EXP^ (-(EC/ (L/D))
Where
E=endurance= 3.54hr
C=sp. fuel consumption
For loiter
L/D=0.866*L/Dmax= 12.2
(W4/W3)=e^ (-3.54*0.822/12.2)=0.787
(W5/W4)= 0.918
(W6/W5)= 0.995
(Wx/Wo)=(W1/Wo)(W2/W1)(W3/W2)(W4/W3)(W5/W4)(W6/W5)=
(0.96) (0.985) (0.77) (0.787) (0.918) (0.995)
(Wx/Wo)= 0.523
(Wf/Wo)=1.06(1-Wx/Wo) = 1.06(1-0.523)= 0.505
(WO)^2=WC+Wp1/ (1-We/Wo-Wf/Wo)
=85000/ (1-0.505-0.405) =192011.36N
Hence first app of forty seater a/c by graphical method is
WO= 192011.36
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Third approximation:
(We/WO)=A WO^cKvs
A=2.36 C= -0.18
Kvs=variable sweep const=1.00 if fixed wing
From second approximation
WO = 192011.36 N
(We/WO)=A Wo^c Kvs=2.36*(5.44*10^5) ^-0.18*1=0.219
Hence overall takeoff wt:
Wo=Wc+Wp1/1-(We/Wo)-(Wf/Wo)=85000/1-0.219-0.470)N
= 194366.54N
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Aerofoil selection
Aerofoil is nothing but the cross section area of wing. The shape
necessary for any wing to produce lift force and hence the prop
selection of aerofoil becomes an important and mandatory step
design.
Aerofoil design is a measure fact of aerodynamics. The aerofoil
completely affected by the flight regime in which the a/c is intended
operate
We know that,
lift=1/2.V^2.CI.S
V stall= 0.25 Vcruise=125km/hr= 37.5 m/sec
For steady and level condition,
L=W
W=1/2.V stall^2.CI max .S
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CI max=2(W/S) 1/.Vstall^2
Where (W/S) =wing loading
CI max= (320*2/ (37.5)2*)2.830
CL max=1.28
Re= V stall. 1/r
Where L is chord length
L=S/AR=54/10.9=4.954
REYNOLDS NUMBER:
R=kinematic viscosity=2.1584*10-5
/sec
Re=0.42*37.33*4.954/2.15*10-5
=3.59*106
So from Reynolds number and CI max we can find the aerofoil NACA
4214, we got the aerofoil NACA4214 as
And for this aerofoil selection the drag co efficient
Cd=0.05
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Thrust calculation:
Thrust is nothing but a reaction force which when acts on bod
produces a motion. It is expressed in Newton. Newtons second law an
third law quantitatively defined thrust together. An aircraft propels wi
the aid of this reaction force. There are three diff independent actio
which causes this reaction to occur
Spinning blades of the propeller or rotating turbine of jet , or th
blast of the propellants in the rocket engine , force a mass of air or gtowards the rear and this mass exerts an equal and opp force on th
system and thus we have a force named , thrust
An a/c with a good propulsion sys design, integrated with a goo
structural char will automatically surprise other phases of design and w
emerge out successfully
We know that
(thrust/wt) takeoff= (thrust/weight) cruse*(Ttakeoff/Tcruise/Wtakeoff)
We know that
(thrust/weight) cruise=1/ (L/D) cruise
=1/12.2=0.0819
We will get
(Wcruise/Wtakeoff) as
(Wx/Wo) = (W1/Wo)(W2/Wo)(W3/W2)
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W1/Wo=0.96Wo
W1=0.97*(191011) =185280.67
W2/W1=0.985
W2=0.985*185280.67
=182501.46
W3/W2=0.818*182501.46
W3=149286.19
As we have to find the fraction of wt at take off to0 the wt at cruise,
Wb/W1=149286.19/185280.67=0.805
(thrust/wt) takeoff= (thrust/wt) cruise*(T take off/T cruise)*(W cruise/W
takeoff)
Thrust=2100kw
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Wing design:
Wings are most important in a/c to generate lift.
The cross section of wing is normally and mostly an aerofoil shape. Th
assures stream lining and reduces the drag.
The design and selection of wing includes chord calculatio
aerodynamic center location, and selection of various angles.
CHORD:It is the line joining from leading edge to trailing edge of an aerofoil,
case of a tapered wing the chord at the root is greater than the chord
the tip.
ROOT CHORD:
It can be determined by evoking the expression.
C root=2S/ b (1)
S=wing area
b=wing span
=chord taper ratio
for low speed subsonic a/c is 0.45
S= (W/W/S)
= (21000/320)=65.625m2
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AR=b^2/S
10.9=b2/65.625
b=26.74m
Root chord (C root)
2S/ b (1+1mda)
=2*65.625/26.74*(1+0.45)
=3.385m
C root= 3.385m
TIP CHORD:
Tip chord can be found from the below expression
=tip chord/root chord
tip chord C tip=root chord
=0.45*3.385=1.523m
ROOT MEAN CHORD:
()=2/3Croot(1^2/(1/))
2/3*3.385(1+0.452/1+0.45)=
()=1.87m
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AERODYNAMINC CENTER (A/D):
It is the point at which the aerofoil where in the coefficient of mome
does not vary with in the change in the angle of attack. Aerodynam
center always lies on the root main chord as a distance of 0.25 from th
leading edge of sub sonic a/c
(A/D)=0.25C root
=0.25*2.99
(A/D)=0.7475m
DISTANCE OF MEAN CHORD FROM THE FUSELAGE CENTER:
The distance () can be cal from the formula
=(b/6)12/1)
=26.74/6*[1+ (2*0.45)]/1+0.45
=5.839
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FUSELAGE DESIGN:
It is hallow and strong tube. It is the main part of the a/c which holds th
crew, cargo and the passenger. It indicates all the parts of the a/c an
holds them up. The fuselage is always streamlined to minimize th
amount of drag produced. The center of the gravity always lies with
the fuselage. This fuselage consists of cockpit where all the a/c contro
are controlled here
As we know
L/b=0.84
L=length of fuselage
b=span
We know
b=26.74
l=26.74*0.84
l=22.46m
As we know the fitness ratio as.
L/d=4.5
d=22.46/4.5
d=4.991m
Length of the empennage of the nose
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=1/10 of length of the fuselage
=1/10(22.46)
=2.246m
DIAMETER OF THE NOSE CONE AND EMPENNAGE:
Lnose/dia nose=1.7
Dia nose=2.246/1.7=1.321m
Length emp/dia emp=1.8
Dia emp=2.246/1.8=1.247m
Wt area:
S reference =C root * dia fuselage
= 3.385 *4.991=16.89m
We know
S=S ref+ S wet
We have seen:
S=65.625m
S wet=S-Sref
=65.625-16.89=48.735m
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Drag and lift estimation:
Like thrust and wt, drag too is a force the thrust produced by the pow
plant, has to overpower those drag force and only by that way the a
can be suspends in the air. Thrust is an aerodynamic force to th
direction of motion.
The drag can be est by the formula
D= (1/2)Vstall^2SCd
Cd is coefficient of drag
CD=CDo=[(CLmax) ^2/(eAR)+
The right hand side has two terms in the eq.the first is parasite drag ter
and the second is the induced drag term.
CDo=CDe*(S wet/S ref)CDe is the effective friction co efficient and its value is 0.003
S wet/S ref=48.735/16.89=2.885
CDo=0.01*2.885=0.02885
CD=CDo+ (CLmax/e AR)
=0.02885+ (1.28/3.14*0.9*10.9)=0.07038
Drag= (1/2) Vstall^2S*CD
=0.5*0.42*37.252*65.625*0.07038=1363.9N
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lift:
The term lift is generally associated with an a/c although lift is als
generated by rotor on helicopter, sails, and keels on the sailboats, an
wind turbines. While the common meaning of lift suggests that
opposes gravity, aerodynamic lift can be in any direction.
We very well know that lift L is given by
L= (1/2)Vstall^2sCLmax
=0.5*0.42*37.332*65.625*1.28
=24581.84N
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Performance:
The evaluation of performance of an aircraft involves of quantiti
such as take off distance, landing distance, rate of climb, climb ang
bank angle, and minimum load factor for turn angle, turn radius, angul
velocity, and endurance. The performance is evaluated with the help
simple parameters like weight, lift and drag coefficients, and engin
thrust characteristics. The formulas used are in the perspective
preliminary design stage of an aircraft. Accurate results require muc
more numerical data.
Take off distance Sto
The distance or the length of the runway required for an aircraft to be a
born success fully is given by the formulaSto = * 1.44 (Wtk)^2+ / (gsCLmax)+ * (T-D) + r (Wo - L) ]
r is the friction coefficient of runway and is usually 0.02
is the density at sea level
T, W, Wtk, WO are in new ton
Sto = [ 1.44*2.8 * 1020 ] / (9.81 * 1.225 * 500.18 * 0.5867 )
[258200 - 10520 + 0.02 *50000 ]
= 1400m
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Hence Sto = 1.4 km
Landing distance SL
The length of the run way required for an air craft to come to a halt afte
it touches is given by
SL = *1.67 ( wl ) ^ 2+ / (gsCLmax ) * (T-D) + R (Wo L )]
Landing weight WL is calculated from the expression below
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WL = WL 30% (WO)
= 1.12 km
Hence , SL = 2.8 km
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Rate of climb Roc and climb angle
Rate of climb is nothing but the rate at which an air craft climbs up whe
it is in pitch up position. The angle at which it climbs in to the
atmosphere is called climb angle
They are given by the following formulaes
Roc = Vcruise * (T-D) / WO
=[520*(1700000-1275000) ] / 1729650
=125.8 m / s
Hence, Roc = 125.8 m / s
Roc = Vcruise sin
Sin =RoC / Vcruise
= sin^-1 (125.8 / 520)
=140
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Bank angle:
The angle between the lateral axis and the horizontal surface of the
earth is called bank angle
It is given by
= cos^ -1 (W/L)
= COS^-1 (0.61 / 1.53)
=66o42
Load factor for turn (nm)
Minimum Load factor required for turn is given by,
Nm = [T/W] * [L/D] where [T/W] is 0.25 from table
=0.25*12.2
=3.05
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Turn angle
The angle with which the aircrafts makes a turn with respect to the
horizontal axis of the earth is called turn angle
Tan = (3.05^2 1 )^0.
=tan ^-1 [3.05^2 - 1] ^ 0.5
=9011
1
Turn Radius R
The radius which the air craft covers a turn is turn radius and is given by
R = Vcruise^2 / [ g* ( nm ^2 1 ) ^0.5 ]
=520^2 / [9.81* (3.05^2 -1) ^ 0.5]
= 9566.06 m
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Endurance E
Endurance is nothing but the
Amount of time spent by the aircraft in air , it is calculated from the
expression
E = ln (WL/Wo)*[(L/D)]
Where (L/D) and C for endurance is 1.6 & 0.4 respectively
= - ln (1.12 / 1.91) * [12.2]
= 6.51 Hrs
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V-N DIAGRAM
The V-n diagram is a graph portraying load factor vs velocity f
given airplane, along with the constrains on both n and v due
structural limitations. The V-n diagram illustrates some particular
important aspects of overall airplane performance.
Load factor aids us in fixing boundaries to an aircraft within which th
aircraft is free to perform and operate. Load factor is dependent o
gravity and hence depending on that we have corresponding on that whave corresponding velocities and eventually V-n plot.
For our calculation, we consider load factors direct proportionality to
the square of velocity. Load factor is given by
n= V2/Vstall
2
Positive load factors indicate that the aircraft is ascending up.
When n=1, V=37.5 m/s
When n=2, V=53.03 m/s
When n=3, V=64.95 m/s
When n=4, V=75 m/s
Negative load factors are experienced by aircraft when it descends dow
When n=-1, V=-37.5m/s
When n=-2, V=-53.03 m/s
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When the velocity is 0, load factor is also zero.
Load factor n=1 gives an initial boundary limit and a dive speed of 200.2
m/s gives final boundary limit.
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The area exposed by continues lines in the plot is the regime in which
the aircraft is bound to perform an operate. The first vertical line
crossing X-axis at 33.33m/s sets the boundary of minimum speed Vmin
The second vertical line crossing X-axis at 200.25m/s sets the boundary
of maximum speed Vmax.
Thus the aircraft can operate between velocities of 37.3m/s an
200.25m/s.
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SUMMARY OF DESIGN FEATURES
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CONCLUSION
Early aircrafts were developed in response to very simple requirement
Today, complex set of requirement like specification of airplane performanc
safety, reliability and maintainability, and other are included. Because t
companies are continuing to try improve on the strategy. In the early days
airplane design, people did not do much computation. The design teams tende
to be small. Modern design projects are so complex that the problem has
examine advertisement for aircrafts; the definition of the best aircraft is vesimple. Aircraft Company sells the fastest, most efficient, quietest, most
expansive airplanes with the shortest field length. Unfortunately such an airpla
cannot exist. As professor Bryson, the father of scientific climatelogy puts it, yo
can only manke one thing best at time. The most expansive airplane would sure
not be the fastest; the most efficient would not be the most comfortable.
Airframe manufacturers are continuously creating innovative design, maki
greater use of new lightweight materials and increasing their focus on passeng
comfort. Achieving a perfect balance between these competing requiremen
represents a tremendous challenge for the design and engineering of t
airframe.
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REFERENCE
The following are the list of the books and websites which helped us to make o
dream a reality and brought our aircraft to life.
Aircraft design-conceptual approach-by Raimer
Introduction to flight-by John D. Anderson
Aerodynamics for engineers- by Arthur and carruther
Aircraft design projects for engineering students B Lloyd and R.Jenkinson
Websites
www.google.com
www.wikipedia.com
www.airliners.com
www.airtoaircombat.com
www.ebookee.com www.nasa.gov.in
http://www.google.com/http://www.google.com/http://www.wikipedia.com/http://www.wikipedia.com/http://www.airliners.com/http://www.airliners.com/http://www.airtoaircombat.com/http://www.airtoaircombat.com/http://www.ebookee.com/http://www.ebookee.com/http://www.nasa.gov.in/http://www.nasa.gov.in/http://www.nasa.gov.in/http://www.ebookee.com/http://www.airtoaircombat.com/http://www.airliners.com/http://www.wikipedia.com/http://www.google.com/ -
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