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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072
© 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 322
Determination of Critical Downforce Coefficient of a Vehicle for
Optimum Aerodynamic Performance
Brightson George1, Jairesh J. V.2, Chithraiselvan G.3, Gokul Nath S.4
1B.E. Student, Mechanical Engineering, Bannari Amman Institute of Technology, Erode-638401
2B.E. Student, Mechanical Engineering, Vins Christian College of Engineering, Kanyakumari-629502
3B.E. Student, Mechanical Engineering, Bannari Amman Institute of Technology, Erode-638401
4B.E. Student, Mechanical Engineering, Bannari Amman Institute of Technology, Erode-638401
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract - - The ultimate aim of every race car designer is
to improve the lap time, without compromising safety and
other aspects. In order to achieve this objective, the most
predominant factor is cornering ability at high speed. During
cornering, the cars havetoreduce itslongitudinalacceleration
to compensate for the lateral acceleration i.e., it has to slow
down while cornering to avoid sliding or deviating from the
desired path, as the traction provided by tyre is limited for a
given load. One such way to improve the cornering ability,
ultimately improving lap time, is by improving the traction of
the tyres by increasing the load acting on it. The effective way
to increase load on tyres while cornering is by increasing
aerodynamic downforce coefficient of a car to a certain limit,
that is, up to critical downforce coefficient. The critical
downforce coefficient is the valueafterwhichthedragnullifies
the positive effect on the lap time caused by downforce. This
paper provides the methodology to determine critical
downforce coefficient of a car for a given track. The critical
downforce coefficient is determined by series of analytical
calculations and simulations carried out using OptimumLap
software.
Key Words: Cornering, Critical downforce coefficient,
Downforce, Drag, Lap time.
1. INTRODUCTION
From a distance, any automobile racingappearstobea sport
which have a strong penchantforpopularityandcommercial
media coverage. But, despite the false facade the highly
popular sport seems to hold, on its root, it act as a place
where new technologies are tested and proved before being
incorporated into the commercial automobiles. In this
technology race, several factors contribute to the win like
chassis design, engine, tyres and so on. Thebestracecarona
track is undoubtedly the fastest car on the track, the one
with the best lap time, at least as long as only single lap is
considered. Since over a race distance several factors come
into play, sometimes it is not the fastest that wins. The time
taken for a race car to complete a lap depends on how fast a
car can accelerate, brake(decelerate), corner ability,
aerodynamics, top speed and so on, of which improving one
compromises another. Of these, aerodynamics is a field
which has attracted a lot of focus over the recent years.
Aerodynamics is the reason why we see more streamlined
cars, and several attachments ranging from small flaps to
large spoilers.
1.1 Significance of Aerodynamics
The importance of building aerodynamically efficient
car is well understood when the effect of aerodynamic
forces on a moving object is analyzed.
Fig - 1 : The cross sections of rod and airfoil with
same drag
In [1], comparison of two cross sectionshows thatacross
section of a circular rod has the same drag as the thicker (up
to 10 times) and larger airfoil. Thus the important step for
any race car is to reduce the drag and thereby increase the
speed and acceleration. However with constrained rules in
the body design of any race car it is almost impossible to
reduce drag below a certain limit. Nevertheless, the drag
reduction is only secondary. The most primary concern of
any race car designer is to produce more downforce as it
would improve the corneringabilityofacarbyincreasingthe
load acting on it.
1.2 Downforce to lap time relation
When increasing the aerodynamic downforce coefficient of
the car, which is done by adding aerodynamic elements, it is
important to note the relatively smaller increase in drag
force or drag coefficient of the car according to [2].Thisdrag
force upon reaching certain value decreases the speedalong
a straight line significantly enough to nullify the positive
effect of increased downforce. Therefore, for very high
downforce coefficient the effect on the lap time due to
enhanced cornering is nullified by the reduction in straight
line performance due to increased drag coefficient. So, for
every vehicle depending on the track an optimum
aerodynamic setting exists and it is marked by critical
downforce coefficient(value above which drag nullifies the
effect on the lap time due to downforce). Throughout this
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072
© 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 323
paper the effect of side winds is not considered. This paper
will provide the methodology to determine the critical
downforce coefficient of a certain vehicle for a given track
(the value varies with different track layouts) using a few
analytical calculations and a series of simulation on the
OptimumLap software.
2. METHODOLOGY
2.1 Selection of Vehicle
Formula SAE-no aero car is chosen for the
determination of critical downforce coefficient as it is
widely known, also, the downforceanddragcoefficient
and other parameters(both performance and
dimensional) of a standard FSAE - no aero car are
available in the online database of the OptimumLap
software. The term no-aero means the car does not
have any aerodynamic add-ons like wings, diffuser,
flaps and so on. Formula SAE is a student design
competition in which students are challenged with the
task of designing, manufacturing and testing a formula
styled race car(open cockpit, open wheel), organized
by SAE International [3]. The competition is all about
selecting the best combination of racing aspects like
braking, acceleration and cornering stability.
Table - 1 : Vehicle configuration of FSAE - no aero
car
The ‘built’ race car is tested for its performance in a
series of events likeAutocross,Skippad,Fueleconomy,
Endurance events. In such competition maintaining a
balance between certain performance parameters is
the key. The real potential of the students is displayed
when they improve a parameter without
compromising another parameter.
Table - 2: Performance metrics of FSAE - no aero
car
2.2 Selection of Track for simulation
The Buddh International Circuit is chosen for the
determination of critical downforce coefficient of the
FSAE car for this paper as the track data, performance
parameters are available in the online database of the
software. The Buddh International Circuit is an
Indian motor racing circuit in Greater Noida, Uttar
Pradesh, India, 40 km from Delhi. It is a very
challenging track characterised by quick change of
directions and fast flowing corners.
Fig - 2 : Buddh International track layout
2.3 Calculation and Simulation:
Initially the data of the Buddh International Circuit is
downloaded from the track database and loaded into the
software from the OptimumLap website. Next load the
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072
© 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 324
parameters of the standard FSAE car with no aero in the
OptimumLap software and the simulation is carried out to
find the lap time. Then the simulation is carried out for
increasing values of downforce coefficient and the
corresponding lap times are noted.
In real world this increase in downforcewouldcorrespondto
the incorporation of aerodynamic add-ons like wings,
diffuser, flaps and so on. As a result, the coefficient of drag
increases with that of downforce, with other values
remaining constant throughout the simulation [4].
The lap time for the FSAE - no aero car with the
initial setup (no aerodynamics add-ons) on the Buddh
International circuit is found tobe139.54seconds.Theinitial
coefficient of drag (Cdo)andcoefficientofdownforce(Cdfo)are
0.6 and -0.01 respectively. The Cdfo is negative which implies
that vehicle experiences lift. In order to carry out the rest of
the simulations we require drag coefficient for every
downforce coefficient we assign.
Relationship between the drag and downforce
coefficients are provided by the equation denoted in [1],
which, to be precise draws the relationship between the
coefficients of lift and drag. Downforce is the negative of lift.
Therefore it is important to note that Cl and Clo are negative
for downforce.
Cd - Coefficient of drag (after aerodynamic add-ons)
Cl - Coefficient of lift (after aerodynamic add-ons)
Clo - Coefficient of lift (before aerodynamic add-ons)= 0.01
Cdo - Coefficient of drag (before aerodynamic add-ons)= 0.6
Cdfo- Coefficient of downforce (before aerodynamic add-ons)
=(-Clo) =-0.01
Cdf - Coefficient of downforce (after aerodynamic add-ons)
=(-Cl)
k - Polar coefficient (ranges from 0.03 - 0.04)=0.04
The equation is solved for increasing values of Cdf
from 0.1 to 2.5 with the Cdf0 and Clo values being -0.01 and
0.6(remains *unchanged throughout) and Cd is tabulated in
the Table - 3.
The value for P is chosen to be 0.04 according to [1] which
accounts for the added drag due to added downforce. The
Cdfo and Cdf are the negatives of Clo and Cl and hence the sign
change.
Table - 3: Cdf to Cd iteration
Cdfo Clo Cdf Cl Cdo Cd
-0.01 0.01 0.1 -0.1 0.6 0.600
-0.01 0.01 0.5 -0.5 0.6 0.610
-0.01 0.01 1 -1 0.6 0.632
-0.01 0.01 1.5 -1.5 0.6 0.689
-0.01 0.01 2 -2 0.6 0.758
-0.01 0.01 2.1 -2.1 0.6 0.775
-0.01 0.01 2.2 -2.2 0.6 0.792
-0.01 0.01 2.3 -2.3 0.6 0.810
-0.01 0.01 2.4 -2.4 0.6 0.829
-0.01 0.01 2.5 -2.5 0.6 0.848
3. RESULTS
Now for every individual set of Cl and (its corresponding) Cd,
the lap time simulation is done on the software and the
respective lap time(s) are calculated. At a certainCl valuethe
lap time reverses its order and starts increasing, which is
Critical Lift coefficient. The lap time is plotted against
downforce coefficient in the graph below. The slope of the
relationship is negative in the beginningandafterthecritical
downforce coefficient it experiences a positive slope.
Chart - 1 : Effect of downforce coefficient in lap
time(i)
From the Chart - 1 and Chart - 2, the critical
coefficient of downforce for the FSAE- no aero car on the
Buddh International circuit is found to be 2.2 and the
corresponding lap time is128.950whichisabout10seconds
clear from the lap time by the initial setup without any
aerodynamic downforce. Going further the critical
coefficient, the lap time increases which is undesirable. So
the aerodynamic add-ons should be designed to reach the
downforce coefficient 2.2.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072
© 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 325
Chart - 2: Effect of downforce coefficient in lap
time(ii)
4. CONCLUSION
To summarize, the initial coefficients of drag and downforce
of the car before any aerodynamic add-ons, which are
usually determined by fluid simulation or wind tunnel
testing, in this case, already present in the database of the
software, are noted. Then for increasing values of the
downforce coefficient the corresponding drag coefficients
are found. For the individual sets of the drag and downforce
coefficients the lap time simulation is carried out. Initially
the lap time decreases but at a certain point it reverses the
direction and increases, the value of the downforce
coefficient after which this increasing trend is shown is the
critical downforce coefficient. In our case, the critical
downforce coefficient is found to be 2.2 and the lap time is
128.950 which is 10 seconds clear from the initial laptime of
the car without any aerodynamic downforce. The difference
at first might seem insignificant but in a race which consists
of the about 20 laps, the difference would become 200
seconds which is enormous and a great advantage over the
others, one that guaranties victory.
REFERENCES
[1] Joseph Katz, “Race car aerodynamics: Design forspeed,”
Cambridge, MA:R, Bentley, 2006.
[2] William F. Milliken and Douglas L. Milliken, Race Car
Vehicle Dynamics, SAE, Inc., 1995.
[3] Danllo Camblaghi, MarcoGadola,Luca Manzo,andDavid
Vetturi, “A tool for lap time simulation,” University of
Brescia. 1996.
[4] Sahil Gupta and Kishal Saxena,“Aerodynamic analysisof
a formula SAE car,” 13th International Conference on
Heat Transfer,Fluid Mechanics and Thermodynamics.

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  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 322 Determination of Critical Downforce Coefficient of a Vehicle for Optimum Aerodynamic Performance Brightson George1, Jairesh J. V.2, Chithraiselvan G.3, Gokul Nath S.4 1B.E. Student, Mechanical Engineering, Bannari Amman Institute of Technology, Erode-638401 2B.E. Student, Mechanical Engineering, Vins Christian College of Engineering, Kanyakumari-629502 3B.E. Student, Mechanical Engineering, Bannari Amman Institute of Technology, Erode-638401 4B.E. Student, Mechanical Engineering, Bannari Amman Institute of Technology, Erode-638401 ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - - The ultimate aim of every race car designer is to improve the lap time, without compromising safety and other aspects. In order to achieve this objective, the most predominant factor is cornering ability at high speed. During cornering, the cars havetoreduce itslongitudinalacceleration to compensate for the lateral acceleration i.e., it has to slow down while cornering to avoid sliding or deviating from the desired path, as the traction provided by tyre is limited for a given load. One such way to improve the cornering ability, ultimately improving lap time, is by improving the traction of the tyres by increasing the load acting on it. The effective way to increase load on tyres while cornering is by increasing aerodynamic downforce coefficient of a car to a certain limit, that is, up to critical downforce coefficient. The critical downforce coefficient is the valueafterwhichthedragnullifies the positive effect on the lap time caused by downforce. This paper provides the methodology to determine critical downforce coefficient of a car for a given track. The critical downforce coefficient is determined by series of analytical calculations and simulations carried out using OptimumLap software. Key Words: Cornering, Critical downforce coefficient, Downforce, Drag, Lap time. 1. INTRODUCTION From a distance, any automobile racingappearstobea sport which have a strong penchantforpopularityandcommercial media coverage. But, despite the false facade the highly popular sport seems to hold, on its root, it act as a place where new technologies are tested and proved before being incorporated into the commercial automobiles. In this technology race, several factors contribute to the win like chassis design, engine, tyres and so on. Thebestracecarona track is undoubtedly the fastest car on the track, the one with the best lap time, at least as long as only single lap is considered. Since over a race distance several factors come into play, sometimes it is not the fastest that wins. The time taken for a race car to complete a lap depends on how fast a car can accelerate, brake(decelerate), corner ability, aerodynamics, top speed and so on, of which improving one compromises another. Of these, aerodynamics is a field which has attracted a lot of focus over the recent years. Aerodynamics is the reason why we see more streamlined cars, and several attachments ranging from small flaps to large spoilers. 1.1 Significance of Aerodynamics The importance of building aerodynamically efficient car is well understood when the effect of aerodynamic forces on a moving object is analyzed. Fig - 1 : The cross sections of rod and airfoil with same drag In [1], comparison of two cross sectionshows thatacross section of a circular rod has the same drag as the thicker (up to 10 times) and larger airfoil. Thus the important step for any race car is to reduce the drag and thereby increase the speed and acceleration. However with constrained rules in the body design of any race car it is almost impossible to reduce drag below a certain limit. Nevertheless, the drag reduction is only secondary. The most primary concern of any race car designer is to produce more downforce as it would improve the corneringabilityofacarbyincreasingthe load acting on it. 1.2 Downforce to lap time relation When increasing the aerodynamic downforce coefficient of the car, which is done by adding aerodynamic elements, it is important to note the relatively smaller increase in drag force or drag coefficient of the car according to [2].Thisdrag force upon reaching certain value decreases the speedalong a straight line significantly enough to nullify the positive effect of increased downforce. Therefore, for very high downforce coefficient the effect on the lap time due to enhanced cornering is nullified by the reduction in straight line performance due to increased drag coefficient. So, for every vehicle depending on the track an optimum aerodynamic setting exists and it is marked by critical downforce coefficient(value above which drag nullifies the effect on the lap time due to downforce). Throughout this
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 323 paper the effect of side winds is not considered. This paper will provide the methodology to determine the critical downforce coefficient of a certain vehicle for a given track (the value varies with different track layouts) using a few analytical calculations and a series of simulation on the OptimumLap software. 2. METHODOLOGY 2.1 Selection of Vehicle Formula SAE-no aero car is chosen for the determination of critical downforce coefficient as it is widely known, also, the downforceanddragcoefficient and other parameters(both performance and dimensional) of a standard FSAE - no aero car are available in the online database of the OptimumLap software. The term no-aero means the car does not have any aerodynamic add-ons like wings, diffuser, flaps and so on. Formula SAE is a student design competition in which students are challenged with the task of designing, manufacturing and testing a formula styled race car(open cockpit, open wheel), organized by SAE International [3]. The competition is all about selecting the best combination of racing aspects like braking, acceleration and cornering stability. Table - 1 : Vehicle configuration of FSAE - no aero car The ‘built’ race car is tested for its performance in a series of events likeAutocross,Skippad,Fueleconomy, Endurance events. In such competition maintaining a balance between certain performance parameters is the key. The real potential of the students is displayed when they improve a parameter without compromising another parameter. Table - 2: Performance metrics of FSAE - no aero car 2.2 Selection of Track for simulation The Buddh International Circuit is chosen for the determination of critical downforce coefficient of the FSAE car for this paper as the track data, performance parameters are available in the online database of the software. The Buddh International Circuit is an Indian motor racing circuit in Greater Noida, Uttar Pradesh, India, 40 km from Delhi. It is a very challenging track characterised by quick change of directions and fast flowing corners. Fig - 2 : Buddh International track layout 2.3 Calculation and Simulation: Initially the data of the Buddh International Circuit is downloaded from the track database and loaded into the software from the OptimumLap website. Next load the
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 324 parameters of the standard FSAE car with no aero in the OptimumLap software and the simulation is carried out to find the lap time. Then the simulation is carried out for increasing values of downforce coefficient and the corresponding lap times are noted. In real world this increase in downforcewouldcorrespondto the incorporation of aerodynamic add-ons like wings, diffuser, flaps and so on. As a result, the coefficient of drag increases with that of downforce, with other values remaining constant throughout the simulation [4]. The lap time for the FSAE - no aero car with the initial setup (no aerodynamics add-ons) on the Buddh International circuit is found tobe139.54seconds.Theinitial coefficient of drag (Cdo)andcoefficientofdownforce(Cdfo)are 0.6 and -0.01 respectively. The Cdfo is negative which implies that vehicle experiences lift. In order to carry out the rest of the simulations we require drag coefficient for every downforce coefficient we assign. Relationship between the drag and downforce coefficients are provided by the equation denoted in [1], which, to be precise draws the relationship between the coefficients of lift and drag. Downforce is the negative of lift. Therefore it is important to note that Cl and Clo are negative for downforce. Cd - Coefficient of drag (after aerodynamic add-ons) Cl - Coefficient of lift (after aerodynamic add-ons) Clo - Coefficient of lift (before aerodynamic add-ons)= 0.01 Cdo - Coefficient of drag (before aerodynamic add-ons)= 0.6 Cdfo- Coefficient of downforce (before aerodynamic add-ons) =(-Clo) =-0.01 Cdf - Coefficient of downforce (after aerodynamic add-ons) =(-Cl) k - Polar coefficient (ranges from 0.03 - 0.04)=0.04 The equation is solved for increasing values of Cdf from 0.1 to 2.5 with the Cdf0 and Clo values being -0.01 and 0.6(remains *unchanged throughout) and Cd is tabulated in the Table - 3. The value for P is chosen to be 0.04 according to [1] which accounts for the added drag due to added downforce. The Cdfo and Cdf are the negatives of Clo and Cl and hence the sign change. Table - 3: Cdf to Cd iteration Cdfo Clo Cdf Cl Cdo Cd -0.01 0.01 0.1 -0.1 0.6 0.600 -0.01 0.01 0.5 -0.5 0.6 0.610 -0.01 0.01 1 -1 0.6 0.632 -0.01 0.01 1.5 -1.5 0.6 0.689 -0.01 0.01 2 -2 0.6 0.758 -0.01 0.01 2.1 -2.1 0.6 0.775 -0.01 0.01 2.2 -2.2 0.6 0.792 -0.01 0.01 2.3 -2.3 0.6 0.810 -0.01 0.01 2.4 -2.4 0.6 0.829 -0.01 0.01 2.5 -2.5 0.6 0.848 3. RESULTS Now for every individual set of Cl and (its corresponding) Cd, the lap time simulation is done on the software and the respective lap time(s) are calculated. At a certainCl valuethe lap time reverses its order and starts increasing, which is Critical Lift coefficient. The lap time is plotted against downforce coefficient in the graph below. The slope of the relationship is negative in the beginningandafterthecritical downforce coefficient it experiences a positive slope. Chart - 1 : Effect of downforce coefficient in lap time(i) From the Chart - 1 and Chart - 2, the critical coefficient of downforce for the FSAE- no aero car on the Buddh International circuit is found to be 2.2 and the corresponding lap time is128.950whichisabout10seconds clear from the lap time by the initial setup without any aerodynamic downforce. Going further the critical coefficient, the lap time increases which is undesirable. So the aerodynamic add-ons should be designed to reach the downforce coefficient 2.2.
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 10 | Oct 2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 325 Chart - 2: Effect of downforce coefficient in lap time(ii) 4. CONCLUSION To summarize, the initial coefficients of drag and downforce of the car before any aerodynamic add-ons, which are usually determined by fluid simulation or wind tunnel testing, in this case, already present in the database of the software, are noted. Then for increasing values of the downforce coefficient the corresponding drag coefficients are found. For the individual sets of the drag and downforce coefficients the lap time simulation is carried out. Initially the lap time decreases but at a certain point it reverses the direction and increases, the value of the downforce coefficient after which this increasing trend is shown is the critical downforce coefficient. In our case, the critical downforce coefficient is found to be 2.2 and the lap time is 128.950 which is 10 seconds clear from the initial laptime of the car without any aerodynamic downforce. The difference at first might seem insignificant but in a race which consists of the about 20 laps, the difference would become 200 seconds which is enormous and a great advantage over the others, one that guaranties victory. REFERENCES [1] Joseph Katz, “Race car aerodynamics: Design forspeed,” Cambridge, MA:R, Bentley, 2006. [2] William F. Milliken and Douglas L. Milliken, Race Car Vehicle Dynamics, SAE, Inc., 1995. [3] Danllo Camblaghi, MarcoGadola,Luca Manzo,andDavid Vetturi, “A tool for lap time simulation,” University of Brescia. 1996. [4] Sahil Gupta and Kishal Saxena,“Aerodynamic analysisof a formula SAE car,” 13th International Conference on Heat Transfer,Fluid Mechanics and Thermodynamics.