Car Aerodynamics & Drag Projects & Experiments
Automotive Aerodynamics & Automobile Drag Coefficients
A truck with added bodywork on top of the cab to reduce drag.
Automotive aerodynamics is the study of the aerodynamics of road vehicles. The main concerns of automotive aerodynamics are reducing drag, reducing wind noise, minimising noise emission and preventing undesired lift
forces at high speeds. For some classes of racing vehicles, it may also
be important to produce desirable downwards aerodynamic forces to
improve traction and thus cornering abilities.
The drag coefficient is a common metric in automotive design, where designers strive to achieve a low coefficient. Minimizing drag is done to improve fuel efficiency at highway speeds, where aerodynamic
effects represent a substantial fraction of the energy needed to keep
the car moving. Indeed, aerodynamic drag increases with the square of
speed. Aerodynamics are also of increasing concern to truck designers, where a lower drag coefficient translates directly into lower fuel costs.
An aerodynamic automobile will integrate the wheel and lights in its shape to have a small surface. It will be streamlined, for example it does not have sharp edges crossing the wind stream above the windshield and will feature a sort of tail called a fastback or Kammback or liftback. It will have a flat and smooth floor to support the Venturi effect and produce desirable downwards aerodynamic forces. The air that rams into the engine bay, is used for cooling, combustion, and for passengers, then reaccelerated by a nozzle and then ejected under the floor.
Automotive aerodynamics differs from aircraft aerodynamics in
several ways. First, the characteristic shape of a road vehicle is
bluff , compared to an aircraft. Second, the vehicle operates very
close to the ground, rather than in free air. Third, the operating
speeds are lower. Fourth, the ground vehicle has fewer degrees of freedom than the aircraft, and its motion is less affected by aerodynamic forces.
Automotive aerodynamics is studied using both computer modelling and wind tunnel
testing. For the most accurate results from a wind tunnel test, the
tunnel is sometimes equipped with a rolling road. This is a movable
floor for the working section, which moves at the same speed as the air
flow. This prevents a boundary layer forming on the floor of the working section and affecting the results.
Drag coefficient (Cd) is a commonly published rating of a car's aerodynamic smoothness, related to the shape of the car. Multiplying Cd by the car's frontal area gives an index of total drag. The result is called drag area,
and is listed below for several cars. The width and height of curvy
cars lead to gross overestimation of frontal area. These numbers use
the manufacturer's frontal area specifications from <http://www.mayfco.com/tbls.htm>
Some examples:
Drag area ( Cd x Ft2)
Relationship to velocity
It is well known that the frictional force of aerodynamic drag increases significantly with vehicle speed.[1]
As early as the 1920s engineers began to consider automobile shape in
reducing aerodynamic drag at higher speeds. By the 1950s German and
British automotive engineers were systematically analyzing the effects
of automotive drag for the higher performance vehicles.[2]
By the late 1960s scientists also became aware of the significant
increase in sound levels emitted by automobiles at high speed. These
effects were understood to increase the intensity of sound levels for
adjacent land uses at a non-linear rate.[3]
Soon highway engineers began to design roadways to consider the speed
effects of aerodynamic drag produced sound levels, and automobile
manufacturers considered the same factors in vehicle design.
See also
References
- ^ [http://books.google.com/books?id=37IHClTXkIEC&pg=PA35&dq=%22automobile+aerodynamics&ei=p0oGR5fPO6bqoQLVvKyqDQ&sig=rHKVxloak0qgjaM2ikon66vxEPA Tuncer Cebeci, Jian P. Shao, Fassi Kafyeke, Eric Laurendeau, Computational Fluid Dynamics for Engineers: From Panel to Navier-Stokes, Springer, 2005, ISBN 3540244514
- ^ Proceedings:
Institution of Mechanical Engineers (Great Britain). Automobile
Division: Institution of Mechanical Engineers, Great Britain (1957)
- ^ C. Michael Hogan & Gary L. Latshaw, The relationship between highway planning and urban noise,
Proceedings of the ASCE, Urban Transportation Division specialty
conference, May 21/23, 1973, Chicago, Illinois. by American Society of
Civil Engineers. Urban Transportation Division
Automobile Drag Coefficients
The drag coefficient is a common metric in automotive design, where designers strive to achieve a low coefficient. Minimizing drag is done to improve fuel efficiency at highway speeds, where aerodynamic
effects represent a substantial fraction of the energy needed to keep
the car moving. Indeed, aerodynamic drag increases with the square of
speed. Aerodynamics are also of increasing concern to truck designers, where a lower drag coefficient translates directly into lower fuel costs.
About 60% of the power required to cruise at highway speeds is taken
up overcoming air drag, and this increases very quickly at high speed.
Therefore, a vehicle with substantially better aerodynamics will be
much more fuel efficient. Additionally, because drag does increase with
the square of speed, a somewhat lower speed can significantly improve fuel economy. This was the major reason for the United States adopting a nationwide 55 mile per hour speed limit (90 km/h) during the early 1973 oil crisis as slower traffic would save scarce petroleum.
CdA
While designers pay attention to the overall shape of the
automobile, they also bear in mind that reducing the frontal area of
the shape helps reduce the drag. The combination of drag coefficient
and area is CdA (or CxA), a multiplication of the Cd value by the area.
In aerodynamics,
the product of some reference area (such as cross-sectional area, total
surface area, or similar) and the drag coefficient is called drag area. In 2003, Car and Driver
adapted this metric and adopted it as a more intuitive way to compare
the aerodynamic efficiency of various automobiles. Average full-size
passenger cars have a drag area of roughly 8.5 ft² (.79 m²).
Reported drag area ranges from the 1999 Honda Insight at 5.1 ft² (.47 m²) to the 2003 Hummer H2 at 26.3 ft² (2.44 m²). The drag area of a bicycle is also in the range of 6.5-7.5 ft².[1]
Automobile examples of CdA ft² are shown below: [2]
Drag in sports and racing cars
Reducing drag is also a factor in sports car
design, where fuel efficiency is less of a factor, but where low drag
helps a car achieve a high top speed. However, there are other
important aspects of aerodynamics that affect cars designed for high
speed, including racing cars. Notably, it is important to minimize lift, hence increasing downforce,
to avoid the car ever becoming airborne and instead force the car onto
the track -- allowing higher cornering speed for the vehicle. Also it
is important to maximize aerodynamic stability: some racing cars have
tested well at particular "attack angles",
yet performed catastrophically, i.e. flipping over, when hitting a bump
or experiencing turbulence from other vehicles (most notably the Mercedes-Benz CLR). For best cornering and racing performance, as required in Formula 1
cars, downforce and stability are crucial and these cars must attempt
to maximize downforce and maintain stability while attempting to
minimize the overall Cd value.
Typical values and examples
The average modern automobile achieves a drag coefficient of between 0.30 and 0.35. SUVs, with their typically boxy shapes and larger frontal area, typically achieve a Cd of 0.35–0.45. A very gently inclined windshield
gives a lower drag coefficient but has safety disadvantages, including
reduced driver visibility. Certain cars can achieve figures of
0.25–0.30, although sometimes designers deliberately increase drag in
order to reduce lift.
Some examples of Cd follow. Figures given
are generally for the basic model. Some "high performance" models may
actually have higher drag, due to wider tires and extra spoilers.
Selected Photographs
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0.7 to 1.1 - typical values for a Formula 1 car
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0.9 -a typical bicycle plus cyclist
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at least 0.6 - a typical truck
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0.51 - Citroën 2CV due to the mudguard, despite the round roof
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0.372 - Ferrari F50, 1996 high drag due to aerodynamic aids and cooling ducts.
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0.36 - Citroën DS, 1955, relative high drag despite the aerodynamic headlights, due to the rough windshield-roof transition.
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0.36 - Citroën CX, 1974 (the car was named after the term for drag coefficient)
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0.355 - NSU Ro 80, 1967 despite the edgy front
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0.35, Audi TT, 1998 [2] much drag despite smooth shape, the similar 2007 version has 0.30 [3]
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0.34 - Ford Sierra, 1982, at least one combi in this gallery! The passat 2003, has 0.32
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0.33 - Citroën SM, 1970 low drag despite edgy front
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0.31 - Citroën AX, 1986 low drag due to down pulled hood
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0.30 - Audi 100, 1983 smooth nose to flow transition
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0.30 - Saab 92, 1947 - developed using wind tunnel testing
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0.28 - Renault 25 TS, 1984, low drag despite its overall edgy shape
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0.26 - Vauxhall Calibra, 1989 even the transition from the bumpers to the head light is smooth
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0.25 - Audi A2 1.2 TDI, 2001, low drag despite wheelarches, due to down pulled hood and fastback
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0.212 - Tatra T77 a, 1935 low drag despite an edgy windscreen-roof transition.
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References
- ^ http://www.lafn.org/~dave/trans/energy/bicycle-energy.html#aero_drag (a bicycle's lower frontal area is offset by a higher drag coefficient)
- ^ http://www.mayfco.com/tbls.htm
- ^ http://www.ent.ohiou.edu/~et181/hpv/hpvplot.html
See also
External links
This article is licensed under the GNU Free Documentation License. It uses material from Wikipedia Encyclopedia article "Automotive Aerodynamics"
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