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Formula Student race car aerodynamic flow visualization
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Project 01

Formula Student Aerodynamic Package Optimization

Genetic-algorithm optimization of the FalconE aerodynamic package, from multi-element wings and diffusers to an 8.15-million-cell full-car CFD study. The report documents ride-height sensitivity, composite manufacture and qualitative rear-wing tuft testing.

Project overview

Component optimization, vehicle-level evidence

Developed a coordinated aerodynamic package for FalconE Racing: a multi-element front wing, four-element rear wing, side diffusers and rear diffuser. Parametric CFD and genetic algorithms explored downforce, drag and component interactions before a vehicle-level study. The portfolio’s previously supplied 1,600+ simulations and 310%+ simulated improvement describe the wider programme; this report does not provide the baseline comparison needed to independently verify that percentage.

8.15M

Full-car CFD cells

553.50 N

Simulated downforce · 22.5 m/s, 30 mm ride height

15 kg

Aero package mass target

01 / Design objectives

Downforce within a constrained package

The design targets were an aero package of no more than 15 kg and 15 m/s (54 km/h) cornering speed. With a 328 kg vehicle-and-driver assumption, a 15 m corner radius and tyre friction coefficient of 1.30, the report calculates 566.8 N required downforce, split 54% front (306.1 N) and 46% rear (260.7 N). These are targets, not measured outcomes.

Eleven candidate airfoils were compared for lift, stall behaviour, angle-of-attack range and manufacturability. Trailing-edge thickness mattered as well as aerodynamic performance; different profiles were selected for different elements rather than assuming one airfoil suited the entire package.

02 / Optimization workflow

Genetic algorithms for nonlinear flow

ANSYS Fluent with k-ω SST supplied the CFD evaluations for sequential multi-objective genetic algorithm (MOGA) studies in ANSYS DesignXplorer, using a controlled-elitism NSGA-II approach. Each stage carried the previous optimum forward. Aerodynamic efficiency throughout these studies means the ratio of downforce to drag (downforce ÷ drag), not an energy-conversion efficiency. A separate custom design-of-experiments study used a Kriging response surface with a stated 5% tolerance.

The three-element front wing underwent three optimization stages: spatial positioning and ground effect (124 design points, 6 iterations), flap chord lengths and angles of attack (436 design points, 7 iterations), and slot gaps and overlaps (211 design points, 8 iterations). Downforce was maximized with a downforce-to-drag ratio above 3; the final section ratio was 6.66.

The four-element front wing also used three stages: ground clearance and flap chord lengths (501 design points, 9 iterations), flap angles of attack (670 design points, 15 iterations), and slot gaps and overlaps (436 design points, 11 iterations). The objective maximized downforce while constraining downforce-to-drag ratio to at least 10. The optimized section ratio was 12.70; the separately studied central element achieved 26.38. These are 2D section results, not full-car forces.

The rear wing combined GOE 447, GOE 448, E423 and NACA 6412 profiles. Three genetic-algorithm stages optimized distance from the headrest and angles of attack (351 design points, 9 iterations), distance and flap chord lengths (402 design points, 10 iterations), then gaps and overlaps (579 design points, 12 iterations). Downforce was maximized subject to a downforce-to-drag ratio of at least 20; the final section ratio was 69.06.

The side diffuser was optimized in a coupled 2D model with the four-element front wing to capture its upwash. A single MOGA study varied inlet height, outlet height, and the horizontal and vertical low-point positions. It evaluated 235 design points over 4 iterations, maximizing combined downforce with downforce-to-drag ratio at least 20. The final section ratio was 36.77.

The rear diffuser used a single MOGA study varying outlet distance, outlet height and tangent angle. It evaluated 420 design points over 9 iterations, maximizing downforce with downforce-to-drag ratio at least 20. The chosen 20° geometry achieved a section ratio of 32.92. Each diffuser result belongs to its modeled section, rather than representing an independently measured vehicle-level load. Design-point counts describe individual optimization runs and are not presented as a grand total of unique CFD simulations; the report does not establish such a programme-wide total.

Parameterized three-element front wing near the front wheel
Figure 01 — Parameterized front-wing geometry and wheel relationship.
Parameterized four-element front wing 2D model with labeled dimensions
Figure 02 — Parameterized four-element front-wing 2D model: clearances, chord lengths, angles, gaps and overlaps.
Velocity contour around the optimized four-element front wing
Figure 03 — Four-element front-wing velocity contour from the section study.
Parameterized rear wing 2D model
Figure 04 — Parameterized four-element rear-wing 2D model and headrest relationship.
Optimized rear-wing pressure contour
Figure 05 — Pressure field around the four-element rear wing.
Parameterized side diffuser 2D model coupled with the front wing
Figure 06 — Parameterized side-diffuser 2D model with inlet, outlet and low-point dimensions.
Side diffuser and front wing coupled velocity contour
Figure 07 — Coupled front-wing and side-diffuser velocity field.
Parameterized rear diffuser 2D model
Figure 08 — Parameterized rear-diffuser 2D model: outlet distance, height and tangent angle.
Rear diffuser velocity contour
Figure 09 — Optimized rear-diffuser velocity field.

03 / Full-car CFD

Resolving wheel wakes and ground effect

Vehicle-level simulations used a symmetric half-car geometry for zero-yaw conditions, with local bodies of influence to refine component interactions and wakes. The enclosure extended 6 m ahead and 15 m behind the car centre, with 7 m height and 5 m width; the report sizes it for blockage below 5%.

The volume mesh contained 8,153,800 cells, with minimum orthogonal quality 0.2001 and no isolated cells. Near-wall sizing calculations explored y+ ≈ 1 using a 0.034 mm first-layer thickness and fourteen layers at 1.3 growth, as well as a cheaper y+ ≈ 40 alternative. These are calculated mesh strategies, not proof that every surface achieved the target y+.

Pathlines and pressure contours were used to inspect front-wing interaction with wheel wakes, underbody acceleration and rear-wing upwash. Residual and force histories document numerical convergence, not experimental validation; force monitors retain fluctuations associated with the separated wake.

Isometric split-car CFD computational enclosure
Figure 10 — Split-car computational enclosure for symmetric, zero-yaw simulations.
Full-car surface mesh
Figure 11 — Surface mesh around the full-car aerodynamic assembly.
Wheel and ground contact surface mesh detail
Figure 12 — Local mesh refinement at the wheel-ground interface.
Wheel and wing surface mesh close-up
Figure 13 — Surface-mesh detail around the wheel and aerodynamic mounting structure.
Underbody and diffuser surface mesh close-up
Figure 14 — Underbody surface mesh resolving the diffuser transition.
Full-car wall y-plus contour
Figure 15 — Reported wall y+ distribution.
Three dimensional full-car velocity pathlines
Figure 16 — Full-car pathlines showing wheel-wake interaction and rear upwash.
Full-car velocity pathlines with rear upwash
Figure 17 — Three-dimensional velocity pathlines showing rear-wing upwash.
Front view of full-car CFD pathlines
Figure 18 — Front-view velocity pathlines around the cockpit and wheel wakes.
Full-car CFD vortex structures colored by velocity
Figure 19 — Full-car vortex visualization colored by velocity magnitude.
Bottom view of underbody velocity pathlines
Figure 20 — Underbody velocity pathlines and ground-effect flow routing.
Top view of vehicle static pressure distribution
Figure 21 — Upper-surface static pressure distribution across the aerodynamic package.
Pressure distribution on the underside of the car
Figure 22 — Underbody pressure distribution from full-car CFD.
Flow separation isosurface showing near-zero axial velocity regions across the car
Figure 23 — Flow separation and recirculation isosurface (near-zero axial velocity) marking drag contributors and local attachment quality across the chassis and wheels.
Isometric view of flow separation isosurfaces around the wheels and wing elements
Figure 24 — Isometric flow-separation isosurfaces highlighting stagnant zones across the wheels, chassis and wing elements.

04 / Vehicle-level results

Ride height changes both force and balance

At 30 mm ride height and zero pitch, the full-car simulation produced 235.51 N downforce at 15 m/s and 553.50 N at 22.5 m/s. Raising ride height to 45 mm reduced those values to 216.15 N and 502.28 N respectively, while shifting the reported centre of pressure forward. These results demonstrate ride-height sensitivity rather than an independently validated lap-time gain.

The 15 m/s simulated downforce is below the report’s 566.8 N cornering target. Section-level loads must not be added to substitute for the full-car result. Future work calls for performance comparisons with and without the package and angle-of-attack adjustments to address understeer or oversteer.

Simulated downforce by ride height

30 mm · 15 m/s · 0° pitch235.51 N
30 mm · 22.5 m/s · 0° pitch553.50 N
45 mm · 15 m/s · 0° pitch216.15 N
45 mm · 22.5 m/s · 0° pitch502.28 N
49 mm · 15 m/s · 0.5° pitch198.12 N
Full-car simulated downforce; common 0–600 N scale.
Ride height (mm)Speed (m/s)Pitch (°)Downforce (N)Drag (N)ClCdCoP from front track (mm)
30150235.51100.033.051.30469.11
3022.50553.50221.043.191.27429.27
45150216.1599.582.801.29381.73
4522.50502.28223.042.891.28374.41
49150.5198.1295.372.571.24374.38

Table 04-01 — Full-car CFD results. Positive downforce and the coefficient convention are retained; these are simulated results.

05 / Manufacture & physical checks

From composite parts to track feedback

The report documents split-mold carbon-fibre wet lay-up and vacuum bagging, with tooling developed through 3D printing, CNC-machined MDF and foam-pattern/fibreglass-mold routes. Internal ribs, bonded joints and mounting hardware translated the optimized profiles into installed components. The rear-wing brackets connected the wing assembly to the chassis and maintained its position and angle. Track testing at Hingurakgoda exposed a bracket failure during reported crosswind gusts up to 90 km/h. Diagonal bracing and revised fillets were subsequently introduced to improve the load path and support the installed wing.

Wool-string tuft testing checked the rear wing’s last two, high-angle elements for flow behaviour. This is qualitative physical evidence, not a measured downforce validation. The report contains no wind-tunnel or instrumented on-track force results; the previously supplied wind-tunnel work belongs to the wider programme and is not verified by this document.

Revised rear wing bracket with diagonal support
Figure 25 — Revised rear-wing support geometry after track-test feedback.
Rear-wing tuft testing photographs
Figure 26 — Wool-string tuft tests on the rear-wing trailing elements.
Manufactured front wing installed on the race car
Figure 27 — Manufactured front-wing assembly installed on the car.