CFD case study no. 9 — Wing CFD and hydrofoil: lift and drag
A wing with a 1.9 m chord at 190 km/h

Lift, drag, lift-to-drag ratio: three numbers, and the picture of the air that makes them.

All the CFD case studies

Wing CFD: reading lift, drag and the pressure around the profile

CFD case study no. 9 of 9. The pictures on this page are screenshots of the HELICIEL CFD tool bench (PRO CFD/BEM upgrade), taken on a real case computed from start to finish: no figure is invented, every value comes from the computation or from the Heliciel designer. No CFD knowledge is needed to read this page. The screenshots show the French interface; the English interface uses the same layout.

Heliciel does not only do propellers, and neither does its CFD: a wing, a hydrofoil, a keel, a stabiliser are drawn and computed the same way. The designer gives lift and drag from the profile polar; the CFD (Computational Fluid Dynamics, numerical simulation of the flow) bench recomputes them on the whole wing, in three dimensions, and above all shows the air around the profile. This case study follows a wing in air; a hydrofoil is treated exactly the same way, only the fluid changes.

wing CFD: vertical pressure cut around the profile, red stagnation point at the leading edge, green suction on the upper surface
The picture every aerodynamics course draws by hand, computed here on the real wing: the red stagnation point at the leading edge, the green suction spreading over the top of the profile, the yellow-orange overpressure underneath. The difference between top and bottom is the lift.

  1. The wing and its flight point
  2. The wing in CFD at three mesh finenesses, three durations
  3. The pressure on the wing and around the profile
  4. The air accelerating over the upper surface
  5. And for a hydrofoil in CFD?
  6. Take-aways

1: The wing and its flight point

Wingwing model shipped with Heliciel, reference chord 1.90 m, reference area 8.6 m² (half-wing, the computation uses symmetry)
Speed52.35 m/s (188 km/h), air at 1.012 kg/m³
Incidencethat of the project, already contained in the exported geometry
Reynolds number5.9 million, Mach 0.15: turbulent and incompressible flow

2: The wing in CFD at three mesh finenesses, three durations

The same wing was computed with the three mesh presets offered for a wing. It is the only decision to take, and this table, drawn from the three runs, says what it buys:

PresetCellsMeshingRunLift CLDrag CDL/D
Fast (1/4)52,0001 min 1030 s0.8860.072112.3
Standard (2/4)198,0003 min 231 min 110.9010.064314.0
Fine (3/4)811,00028 min 305 min 090.9060.060115.1

The reading is crystal clear: the lift hardly moves from one preset to the next (2 % between the first and the last), the drag drops at each step (−17 %), and the lift-to-drag ratio rises with it. A coarse mesh overestimates the drag: it does not describe finely enough the thin layer of slowed air sticking to the skin of the wing. For a lift, the fast preset is enough; for a drag or a lift-to-drag ratio, the fine preset is needed, and it counts in half-hours.

CFD results panel of the wing: lift and drag coefficients, lift-to-drag ratio, flow conditions
The results panel of the fine run: CL 0.906, CD 0.060, L/D 15.1, i.e. 10,795 N of lift for 715 N of drag. Below, the flow conditions and the recall of the preset used.

3: The pressure on the wing and around the profile

upper surface of a wing in CFD: blue suction over the whole top, red leading edge
The top of the wing, seen in perspective from the tip. The whole upper surface is blue: in suction. The leading edge is red: this is where the air strikes. The orange wireframe cylinder is the bench's incidence zone marker, it is not part of the result.

The pressure cut at the top of the page completes this view: it shows that the suction does not stay stuck to the skin but extends into the air above the wing, over a thickness comparable to the chord. A wing lifts because it lowers the pressure of a large volume of air above it, not only at its surface.

4: The air accelerating over the upper surface

vertical velocity cut around a wing profile: red acceleration over the upper surface
The same cut, coloured by velocity. The air arrives at 52 m/s (green). Above the wing it accelerates to more than 80 m/s (red): it is this acceleration that makes the suction of the previous picture. Under the wing, it hardly slows down.

wing in CFD with surface pressure and streamlines
The streamlines over the surface pressure: they follow the wing without separating. At this incidence, the flow is healthy over the whole span. A stall would show here as lines moving away from the skin and curling behind the trailing edge.

5: And for a hydrofoil in CFD?

Nothing changes in the approach. Heliciel ships a hydrofoil model; the fluid becomes water, about a thousand times denser than air, and the loads change scale: this is why a foil of a few square decimetres is enough to lift a boat. The CFD bench takes the fluid of the project, with its density, viscosity and vapour pressure, and the reading of the minimum pressure becomes, as for the boat propeller, the cavitation question: if the darkest blue of the upper surface drops below the vapour pressure, the foil cavitates.

6: Take-aways

The CFD case studies

« Previous: Ducted fan CFD: duct and radiator

  1. Understanding a CFD result in five pictures
  2. Boat propeller CFD: thrust and pressure on the blades
  3. Aircraft propeller CFD: cruise and static thrust
  4. Drone propeller CFD: hover
  5. Wind turbine CFD: power and wake
  6. Tidal turbine CFD: a 16 m rotor in the current
  7. Ducted fan CFD: duct and radiator
  8. Wing CFD and hydrofoil: lift and drag (you are here)

These case studies complement the Heliciel design tutorials (in French), which cover the BEM side: blade design, choice of speed, performance curves. To go further into the method, the technical collection of twenty tutorials remains available.