Summary
The
following report is a detailed yet concise description of a design for the
construction of a supersonic transport vehicle. The report begins with an introduction of the vehicle, motive for
the design, and basic characteristics that make the design distinctive.
Following the introduction is a
section outlining the Mission specifications and giving the account of a
typical mission that the aircraft should undergo. Next calculations for the Take Off Weight are displayed, with
assumptions and preliminary estimates of various values mentioned. Wing loading, area, and aspect ratio are
also exhibited with details and explanations of how we arrived at the values.
The specific engine our team selected
to power our aircraft is declared in the next section. Elucidation of the choice and some important
information about the engines is written.
Next is a section detailing the
aerodynamics and performance of the aircraft.
Properties include speed for minimum drag, stalling speed, required
thrust, and takeoff field length information.
Graphs are plotted to show relation of various values and for use in
calculations.
Fuel weight and volume is given with
calculations as well as the range of the aircraft at full fuel load. A refined Estimate of Structural Weight
available for building the aircraft is specified and charts are used to reveal
weight distribution. Next wing shape,
fuselage dimensions, and a detailed description of landing gear dimensions and
placement are featured. The report is
finished off with a three-view illustration of the aircraft.
The report largely endeavors to illustrate how the design
meets the stated requirements and is able to achieve a typical mission
successfully.
Team
summary
Adam made several initial assumptions and comparisons using the research of similar aircraft to sort of kick start the project. His initial work provided some framework to work with in getting together initial values. Siddharth expanded on these to come up with several calculations and values. All team members met to discuss and work on calculating various values for aerodynamic performance and properties of the aircraft many times. Eventually the team delegated certain responsibilities to each team member. Each person was responsible for making sure the calculations for his set of properties of the aircraft were correct, double checked, and put in final form. All team members contributed to all of these at some point, but individuals were responsible for these parts on the final report. It broke down more or less like this:
Tim –
Basic specifications
such as;
Take Off Weight
Weight fractions
Payload
Wing loading, area,
aspect ratio
Mission Specification
and Typical Mission Profile
Siddharth –
Fuel weight and volume
Range at full fuel load
Structural weight
Wing geometry
Fuselage Dimensions
Landing gear dimensions
and placement
3-view of the aircraft
Adam Plondke -
Speed for minimum drag
Stalling speed
Thrust
Takeoff field
Selection of engines and
justification
Graphs
and charts, empirical data for assumed values
Adam put together word files for the final
report. Tim proof read, checked over,
and further organized/compiled the report.
Tim also wrote the summary and introduction for the final report. Although it was hard to get three people
together sometimes due to different schedules, the team found many times it
could meet or two could meet to work on the project. No one missed a meeting that they said they could come to. All team members feel very good about the
contribution of the others to the project.
Contents
Summary-------------------------------------------page1
Team Summary-----------------------------------2
Contents--------------------------------------------3
I Introduction----------------------------------------4
II Mission Specifications---------------------------5
III Typical mission profile--------------------------5
IV Basic specification of our SST-----------------6
V Assumptions
made-------------------------------7
VI Selections of
engines----------------------------8
VII Speed for minimum drag------------------------9
VIII Stall
speed-----------------------------------------11
IX Thrust required and thrust
available-----------12
X Graph of thrust vs.
speed------------------------13
XI Graph of thrust vs.
altitude----------------------14
XII
Takeoff field length------------------------------15
XIII Graph of runway length vs.
altitude------------16
XIII Fuel Weight and Volume------------------------17
XIV Refined value for the structural
weight--------18
XV Wing Shape----------------------------------------19
XVI Fuselage dimensions------------------------------20
XVII Landing gear and placement---------------------20
XVIII Multiviews of the aircraft------------------------21
XIX Addendum------------------------------------------21
XXI Calculations-----------------------------------------22
XXII Sources
used----------------------------------------23
Introduction:
This
is a conceptual design for a supersonic transport vehicle. Our team chose to develop this design after reasoning
that the only Super Sonic Transport (SST) in operation, the Concorde, was
manufactured over two decades ago and recent developments by the aviation
industry in the fast paced era in which we live warrant something newer and
better. Cutting edge technology allows
us to ameliorate previous designs and build a modern SST that is faster and
more efficient. We are able to design
an aircraft that can carry up to 300 passengers, three times as much as the
Concorde, and even more importantly, a supersonic airliner that is affordable
for the average person. Being that the
design is intended for commercial use, concerns such as airport accessibility
and safety have also carried over into the final design.
The
Mission necessitates the following specifications:
Ø Aircraft must be
able to carry 300 passengers, their luggage, and their supplies.
Ø Aircraft must
have a range of 8000+ miles.
Ø Aircraft must be
able to cruise at Mach 3 over an extended period of time.
In addition the following constraints have been imposed:
Ø Aircraft must be
able to take off with three engines.
Ø Aircraft must be
able to survive an engine failure anywhere
Ø Enough fuel reserve
to be diverted to an airport 300 miles away from last stage of the landing
approach, including a 1 hour loiter
A typical mission profile:
Our
Aircraft will take off with a maximum payload and full fuel tank from Los Angeles
airport and climb to 60,000 feet. The aircraft will then cruise at Mach 3 for a
distance of 7,900 miles. When approaching the runway at Melbourne, Australia
the aircraft will loiter for an hour in the air before landing. At this point
the SST must have enough fuel to be diverted to an airport 300 miles away in
the case of an emergency.
To estimate take Off Weight we first had to find the payload and
the payload fraction. Referring to the
mission specifications it is evident that the payload carried by the aircraft
will be the combined weight of 300 passengers plus their luggage plus 5 tons of
cargo. In addition, it must carry the
crew, which will consist of 12 members. We assumed that the average mass of
each passenger would be 117.2 Kg. The
average weight of luggage per passenger was assumed to be equal to 31.8 kg. The
mass of supplies provided for per passenger (food, drink, etc.) was calculated
to be 3.8 Kg. The total payload is 408029.5 N.
The calculation is shown as follows:
(Weight of
passengers + weight of cargo) * (300 + 12) = 408029.5 N
5 tons of cargo =
49,000 N
359,029.5 N
+
49,000.0 N
408,029.5 N
The payload fraction was assumed to be .1 from comparisons to
similar aircraft.
Now to find Take Off Weight
we divided the payload by the payload fraction:
TOW = Payload = 3,550,213 N
W = 3,550,213 N =
4240.12 N/m2
We
assumed a suitable wingspan to be 51.83 m, based on comparison to similar
aircraft. To calculate Aspect Ratio we divided the square of
the wingspan by the surface area of the wing:
b² = (51.83
m)² = 3.208
S 837.29 m²
The engine we selected is the JSF-119,
which had a thrust of 40000 lbs per engine.
The following assumptions were made while we designed our
aircraft. They are as follows –
Note: Almost all the values were based on data acquired from
similar aircraft and/or extrapolations of graphs.
Our SST requires engines that are capable of flying for extended periods of time at Mach 3, but it also requires enough thrust for steady level flight. To get an estimate of the thrust required at takeoff, we assumed a value of 0.3 TOW. None of the engines we looked at initially seemed to be able to provide the thrust we required. The few engines that appeared suitable possibilities were the turbofan engines designed for the Boeing 777.
The problem was that the engines designed for the 777 were too big and heavy to be used for our aircraft. Such big engines would have created an enormous amount of drag, which would greatly affect the efficiency. Moreover, these engines were designed for airplanes that had a cruising speed of Mach 0.85 while our SST had to fly at a much higher supersonic speed (Mach 3).
The engine we finally decided on was the Pratt and Whitney JSF – 119 engine. As the name implies, the engine was designed for the Joint Strike Fighter. The thrust that these engines provide is 40,000 pounds each. As we have a total of four engines, the total thrust provided by these engines is 160,000 pounds, which satisfies our requirements.
The value for TSFC was taken as 0.52. This was based on the few details provided by Pratt & Whitney and also on educated estimates. The reason for this is that usually TSFC is calculated from thrust and fuel flow rate, a quantity we did not have. However, we found the fuel flow rate from the thrust and the TSFC.
The bypass ratio (the ratio of the mass of cold air leaving the engine to the mass of hot air) wasn’t available for this engine on the Pratt & Whitney page but we assume that it is very close to one.
The placement of the engines is approximately half the way along the wing. A more detailed explanation for placement of the engines is provided later in this paper.
Speed for minimum drag
The
speed for minimum drag is when L = W
Therefore
the equation for minimum drag speed is:
Uinf^2
= 2W/(rho*S*Cl)
Substituting:
Uinf^2
= 2*4080301N
/rho * 837.29 * .107174
Uinf
= sqrt [8160602/rho *89.73571846]
As these graphs show, the speed for minimum drag increases as the altitude increases.
Stall Speed
Vs^2
= 2*W/rho S Clmax
Substituting:
Vs
= sqrt (8160602/rho 837.29 Clmax)
There are two different plots because a range of 1.6 to 1.8 was given as CL max.
Thrust
required and Thrust available
Drag
= Cdo + Cdi
Cdi = .0009077
Cdo
= .011/(Minf^2 –1)
CD
= (.011/(Minf^2 –1))+.0009077
D =
.5*rho*Uinf^2*S*CD
D =
.5*rho*Uinf^2*837.29*((.011/(Minf^2 –1))+.0009077)
D =
rho*Uinf^2*837.29*((.011/(Minf^2 –1))+. 0009077)
at
low speed D = rho*Uinf^2*837.29*.0119077
At
min drag speed
These graphs show that the required thrust will equal to
the available thrust at about 1000 m/s and altitude 2000m. Steady
level flight beyond this point is impossible because the required thrust
exceeds the available thrust
Takeoff
field length
Runaway
Length = (1.2*Stall speed)^2/ net acceleration
Net
acceleration at takeoff = net Thrust/ mass of aircraft
= / 4080301= 2.646 m/s
The calculation for the fuel weight was based on the mission specification that the aircraft must be able to travel about 8,000 miles. In addition to this, the SST should be able to fly an additional 300 miles in the unforeseen circumstance that it should be diverted to another airport. We also had to take into consideration the fuel that needed to be burned to reach the desired cruise altitude of 60,000 feet. We assumed this to be an extra ten percent of fuel weight.
Distance
flown per pound of fuel = V/(c * D)
Where
V
= velocity of the aircraft = 1980.58 mi/hr
c = specific fuel consumption at
cruise altitude = .52 lbs of fuel per pound of thrust
Per hour
D = Total Drag at cruise altitude
= 33227.63 pounds
But
as our cruise range is 8300 miles we get fuel required as –
In
addition we will add an extra ten percent of fuel weight that will be required
to attain the cruise altitude of 60,000 feet
Hence
we arrive at the fuel fraction = weight of fuel/takeoff weight = 38.7
%
The
density of aviation fuel is around 790-kg/cubic meter
The
weight of fuel in kg is 161334.59 kg
As seen in the previous page, the fuel fraction was 38.5 percent. The payload fraction was approximated as 10 percent based on airplanes of similar designs. The average weight of the four engines can be approximated as 15 percent of TOW. Hence the remaining weight of the aircraft can be attributed to the structural weight. Hence a refined value for the structural weight fraction will be 36.5 percent.
Aircraft component |
Percentage of Aircraft Weight (TOW) |
Fuel |
38.7 |
Engines |
15 |
Payload |
10 |
Structure |
36.3 |
The distribution of the weight of the aircraft can be visualized best from the following pie chart –
One might notice that the structural weight is a little higher than usual. This value for structural weight allows us to experiment with more stronger and heavier alloys for the frame of the airplane. We must also take into consideration that as our aircraft will be cruising at Mach 3, a sufficient amount of material with high thermal resistance and coefficient of thermal expansion should be incorporated to protect the airplane from the adverse heating affects of high-speed flight. Such materials will only add to the overall structural weight of the aircraft. Hence a higher percentage of the weight of the aircraft must be devoted to the structure.
The fact that our aircraft needs to cruise at an extremely fast velocity is reason enough for a high degree of sweep on our airplane. The reason for this is to reduce the resultant velocity with which the air hits the wing. The higher the sweep angle, the lower is the effective velocity and the heating effect of air friction, a very important aspect.
After it was decided that a high angle of sweep was
an absolute requirement, we had to decide on the whether we should sweep the
wings forward or backward. Using rough dimensions, we calculated the center of
mass for the aircraft for a forward sweep and a backward sweep using the mass
properties of the Mechanical Desktop software. We found that with a forward
sweep, the center of mass of the aircraft was too close to the front and this
would make the aircraft highly unstable. Consequently, it was decided that a
backward sweep was the best solution.
Another problem that needed to be tackled along the
way was the extremely high value for the platform area (837.29 square meters).
Using conventional swept-back wings would have meant that our wingspan would
have been extremely large. Such a large value for wingspan would have meant
that we would be unable to use a vast majority of the airports in the world, as
they can’t accommodate planes with very large wingspans.
The necessity for a swept wing and the limitation
for an acceptable wingspan led us to the conclusion that the best alternative
was a Delta Wing. The Delta wing could provide us with a large platform
area and high sweep but at the same time provide us with smaller wingspans as
compared to normal swept back wings.
In fact, when we did a comparison with similar
planes such as the Concorde, the Boeing 2707 SST and the Tupolev Tu-144, we
found out that all employed Delta Wings.
Using estimations based on extrapolations of the
attributes of other aircraft, we found out that an ideal wingspan would be in
the vicinity of 170 ft (51.83 square meters). Using this value, the altitude of
the wing would be 32.30 meters.
The aircraft was designed to carry 300 passengers, their
luggage and limited cargo (5 tons). Taking all these parameters into
consideration, we decided the approximate length of the aircraft to be 65
meters. The average cross-sectional diameter of the aircraft will be 5 meters.
As mentioned earlier, the wingspan will be about 51 meters.
The angle of sweep for the wings will be around
38.55 degrees. The distance from the base of the wing to the tip will be about
32 meters. The average wing thickness will be about .25 meters.
Another point to note is that the front wheels will
have a larger diameter and will be thicker than the rear wheels. This is to
sustain the greater load placed on the front wheels. The rear wheels have a
diameter of 0.75 meters while the front wheels have a diameter of 0.90 meters.
The average thickness of the tail wings will be
0.125 meters. The height of the tail will be 5 meters and its average thickness
will be 0.2 meters.
The landing gear will extend 4 meters to the ground.
In addition the exit hatches will be 1.5 meters above this level. Hence the
gate will be 5.5 meters above the ground, which in turn corresponds to the
second level of most buildings.
The rear landing gear will be approximately 14
meters from the axis of the plane on each side and about 5 meters in front of
the rear of the wings.
The front
landing gear will be on the axis of the plane and will be about 5 meters ahead
of the front of the wings.
The engines will be placed exactly in between the
rear landing gear and the axis on either side.
The wingspan will be 51 meters, which allows the
plane to land in virtually any airport.
Note: The following views were created with AUTOCAD (Mechanical Desktop 3).
The engines have been hidden to show a better view of the landing gear. The engines are positioned as mentioned in the previous page.
The multiviews were done according the American Standard of Third Angle Projection.
The isometric drawing was included to give a better overall idea of our SST.
Addendum
–
The following material was used to estimate various quantities.
Airplane |
# of Passengers |
Max TOW lbs |
TOW Kg |
Max TOW N |
Range mi |
Wing span m |
Wing Area ft^2 |
Wing area m^2 |
NASA TCA |
310 |
738,550 |
334,932 |
3,282,338 |
|
|
|
0 |
Tu-244 |
300 |
771,625 |
349,932 |
3,429,333 |
5,716 |
|
12,916.70 |
3937.01016 |
S-21 |
10 |
114,200 |
51,790 |
507,539 |
|
|
1,506.90 |
459.30312 |
Concorde |
100 |
408,000 |
185,028 |
1,813,274 |
3,180 |
26 |
3,856.00 |
1175.3088 |
S-51 |
68 |
195,105 |
88,480 |
867,105 |
5,715 |
|
3,230.00 |
984.504 |
Boeing SST |
300 |
600,000 |
272,100 |
2,666,580 |
3,900 |
37 |
9,000.00 |
2743.2 |
Tu-144 |
140 |
414,000 |
187,749 |
1,839,940 |
4,000 |
29 |
|
|
Calculations
Payload Fraction |
0.1 |
|
|
|
|
Average Passenger mass (kg) |
81.8181 |
|
|
|
|
Average luggage mass per pass.(kg) |
31.8181 |
|
|
|
|
Supplies mass per passenger (kg) |
3.786 |
|
|
|
|
Total Mass per passenger (kg) |
117.4222 |
|
|
|
|
Max Passengers + crew |
312 |
|
|
Passengers |
300 |
Max Payload (kg) |
41635.73 |
|
|
Crew |
12 |
Acceleration Due to gravity (m/s^2) |
9.8 |
|
|
Cargo (Kg) |
5000 |
Weight of Max Payload (newtons) |
408030.1 |
|
|
|
|
Takeoff weight (newtons) |
4080301 |
|
|
|
|
Wing area (square meters) |
837.29 |
|
|
|
|
Wing Loading (n/m^2) |
4873.223 |
|
|
|
|
Wing span (meters) |
51.83 |
|
|
|
|
Aspect ratio |
3.208385 |
|
|
|
|
Gamma |
1.4 |
|
|
|
|
Cruise Mach Number |
3 |
|
|
|
|
Cruise Altitude (Meters) |
18292 |
|
|
|
|
Air pressure at cruise altitude (N/m^2) |
7217.5 |
|
|
|
|
Dynamic pressure at cruise altitude |
45470.25 |
|
|
|
|
Lift Coefficient |
0.107174 |
|
|
|
|
Angle of attack (radians) |
0.303134 |
|
|
|
|
Max. Lift Coefficient at takeoff |
1.6 |
|
|
|
|
Density at zero altitude (kg/m^3) |
1.225 |
|
|
|
|
Stall Velocity (m/s) |
70.51721 |
|
|
Stall Velocity (km/h) |
253.862 |
Takeoff Velocity (m/s) |
84.62065 |
|
|
Takeoff Velocity (km/h) |
304.6343 |
Thrust at Takeoff (Newtons) |
1224090 |
|
|
|
|
Spanwise efficiency factor |
0.95 |
|
|
|
|
Induced drag coefficient |
0.0012 |
|
|
Coefficient of Parasitic Drag |
0.011 |
Speed of sound at cruise altitude (m/s) |
295.07 |
|
|
Cdo at cruise speed |
0.003889 |
Air density at cruise altitude |
0.11606 |
|
|
Parasitic Drag |
148070.6 |
Induced drag (newtons) |
45670.85 |
|
|
|
|
Number of engines |
4 |
|
|
|
|
Average thrust per engine at takeoff (N) |
306022.6 |
|
|
|
|
|
|
|
|
|
|
Net Thrust at takeoff (newtons) |
1101681 |
|
|
|
|
Mass of airplane in kg |
416357.3 |
|
|
|
|
Specific Range (mi/lb) |
0.025723 |
|
|
|
|
Fuel required (lbs) |
322669.2 |
|
|
|
|
Range (miles) |
8300 |
|
|
|
|
Extra fuel required to attain cruise altitude (lbs) |
354936.1 |
|
|
|
|
Extra fuel required to attain cruise altitude
(newtons) |
1581079 |
|
|
|
|
Drag at cruise (Newtons) |
148070.6 |
|
|
|
|
TSFC (lb/lb.hr) |
0.52 |
|
|
|
|
Fuel fraction |
0.387491 |
|
|
|
|
Sources
Used
1. Jane’s all the World’s Aircraft
2. Fundamentals of Flight – Richard S Shevell
4. Http://www.pratt-whitney.com