yokebutt said:Anders,
Is that also true of the same section without camber? Or is that why cambered foils have their low-drag bucket shifted? Please explain!
It is no clearcut answer so here goes...
Some important terms:
Angle of Attack: The angle between the airflow and the mean cord of the foil.
Lift: The force perpendicular to the flow of air
Drag: The force in the same direction of the airflow.
Cl: lift coefficient. A non dimensional number describing how much a lift a foil creates. To get the actual lift force you use:
Lift= cl*density*area*(velocity^2)/2
Cd: drag coefficient. same as lift coefficient but describes the drag.
Stall: When the flow no longer can follow the foil smootly. Instead a wake of turbulent air is created. (Like the suction area behind a lorry) At a certain angle of attack any foil starts to stall. When a foil stalls the lift decreases and the drag increases.
If there was no drag all foils would create a net force perpendicular to the airflow. The drag shifts the net force so it is angled slightly along the air flow
the angle can be calculated by:
drag angle=arctan(Cd/Cl)
See picture in my previous message
The Cl/Cd ratio are the non-dimensional version of the Lift/Dag ratio.
If a foil creates a forward net force as seen from the coordinate system of the foil depends on both angle of attack and dragangle. If drag angle is less than the angle of attack then the net force is forward.
For the NACA 0012 (The uncambered version of NACA 6412) the drag angle is 5 degrees (arctan(0.074/0.87)) at an angle of attack of 10 degrees. This means that this symetrical foil have a net force directed forward.
As understood from the above (hopefully) Cl and Cd and therefore the drag angle are not fixed numbers for a foil but depends on angle of attack. For every foil there is a certain angle of attack that gives the lowest drag angle.
A cambered foil is simply put a bent symetrical foil. A symetrical foil has its lowest drag (and lift=0) at 0 angle of attack. A cambered foil has a leading edge that will be straight towards the oncoming flow at a angle of attack different from 0 and have low drag around this angle. This shifts the bucket and gives a higher cl/cd ratio and therefore a lower minimum drag angle.
But remember that the foils I have shown are 2D foils. Real 3D foils have higher drag than their 2D counterpart (due to induced drag but thats another story). For a 2D foil the Cl/Cd ratio can easily be 50 or more, a 3D wing around 20, but a sail have a Lift/Drag ratio of around 6. A Lift/Drag ratio of 6 means a drag angle of 9 degrees. This drag angle is so high that the net force is more or less perpendicular to the mean cord of the sail.
Sails have a maximum Lift/Drag ratio at an angle of attack that is lower than the angle of attack of maximum lift, just before stall. Going to windward the lift/drag angle is important since it can be shown that this ratio directly affects maximum velocity made good.
C A Marchaj mentions in "Sail Performance" the interesting effect of pumping with the sheet to create "negative drag" by using unsteady flow effects.
I hope this gave some explanation. (And that it is in its essenssials correct. I´m not an aerodynamics expert just a physicist interested in sailing.)
Anders M
PS Had to check that normal is an english term and not a swedish after your reply. Hope I avoided any more strange terms, its so easy to write swenglish.