Lift is actually the result of normal pressure and shear stress distributions all over the wing surface. This is a result of wing geometry, angle of attack, speed of the oncoming air, etc. There is a Newtonian explanation (Conservation of Mass, Momentum and Energy which together result in the famous Navier-Stokes partial differential equations), an explanation relating lift generation to the
circulation of air around the airfoil (Kutta-Joukowski Theorum) and the Bernoulli explanation which we're all the most familiar with.
The Bernoulli equation works great and it's true that when air over the top of the wing speeds up the pressure goes down. The problem with this explanation is when people start spouting the "Equal Times" explanation, where they say "the air going over the top of the wing has to catch up to the air below it, and the path it travels is longer because the top is curved and the bottom is not, so it has to speed up and thus the pressure on top drops because of Bernoulli!" <-- The end is correct, the rest is bullcrap.
The truth is the air at the bottom never catches up to the air at the top, and here's a
great animation of what actually happens. A better explanation of why the air speeds up on top is a physical geometric one. All those parallel lines of air are called "streamlines," and when the streamlines are diverted over the top of the airfoil they bunch up and squeeze closer together until they pass the trailing edge. The Conservation of Mass equation does say the same amount of mass has to leave out the back as what comes in the front (just not that the top and bottom have to exit at the same time), so as those streamlines bunch up the
area between them decreases and the only way to satisfy conservation of mass is to speed up the air. Bernoulli then tells us that increase in the speed must decrease the pressure. An easier physical analogy is the venturi in a carburetor, because its actual walls contract, speeding up the air in the throat (and thus decreasing the pressure) because of Conservation of Mass (the same amount has to go out the back as what comes in the front). When the throat widens up again and its area increases, the air slows back down to its original speed at entry.
This relationship between air velocity and area is explained mathematically by the
Continuity Equation: V1A1 = V2A2
(assuming incompressible flow which means we can neglect air density)
The streamlines bunching together on the upper surface of the airfoil is analogous to the venturi example, only instead of physical walls constricting the air it is the streamlines of other flowing air above and its momentum that act as a barrier. The result is the same:
Area goes down so
velocity must go up (continuity equation).
Velocity goes up so
pressure must go down (Bernoulli equation).
So why can an asymmetric airfoil fly upside down?
I was curious about this myself. I knew the answer lay somewhere in the wing geometry and the deflection of the oncoming air (angle of attack = angle between the chord line and the free stream oncoming air). When you fly inverted you have to shove a lot of forward stick to maintain level flight, and furthermore you have to shove a lot more forward stick in say a Cessna with a flat-bottomed airfoil than you would in an Extra 300 with a symmetrical airfoil (this is assuming you don't mind the engine stopping on the Cessna!). Why is this? And come to think of it, why does the symmetric wing on the Extra generate lift at all (even upright), and why do you need a greater pitch angle to keep it in level flight?
I hit the jackpot and found an outstanding article titled
An Aerodynamicist's View of Lift, Bernoulli and Newton, written for The Physics Teacher magazine by Charles N. Eastlake - an Aerospace Engineer
and a pilot.
Eastlake explains inverted flight and symmetric wings on pages 6-7 of the document (pp. 171-172), and I recommend checking out figures 3, 4 and 5. He says the key to all these questions is the location of the
stagnation point. The stagnation point is the point on the airfoil where the oncoming air velocity=0 - on the leading edge the air has hit a wall and has to split two ways, above the wing and below it. There is also a stagnation point at the tip of the trailing edge, because the leading edge blocks any oncoming air from hitting it.
In all three cases of the flat-bottom airfoil, the symmetric airfoil and the inverted airfoil, the stagnation point at the leading edge is is located in a different place. In the first two cases the stagnation point is on the lower surface of the airfoil... but on the symmetric airfoil it's farther from the chord line on the bottom of the wing. This is why you need more aft stick to keep the nose up and maintain altitude with a symmetric airfoil, because you are basically tricking the wing into putting the stagnation point in such a place that the air flowing over the top is forced through more deflection and a resulting narrower path of bunched streamlines.
In the case of the inverted wing, you are pushing stick forward so that the oncoming air actually hits the
top of the airfoil, not the bottom. With the resulting stagnation point on the upper surface of the wing, the air that splits over the leading edge and turns to follow the lower surface faces more deflection and the streamlines bunch up on the
lower surface of the wing, not the upper. Thus we have actually tricked the air into thinking the top of the wing is the bottom, and the bottom is the top! The wing flies along normally upside with the high and low pressure areas exactly opposite of where we are taught they should be.
Thus even though the shape of a flat-bottom airfoil helps create more efficient lift,
we the pilots are ultimately the ones in control of the constantly changing shape of the pressure distribution over the wing, by controlling angle of attack, airspeed and wing geometry (with things like flaps and slats). For every wing shape attempted there are graphs showing AOA vs. Lift Coefficient (CL). For every AOA there is a corresponding value for CL, and they are all different! When you start adding flaps to the mix, you get a different curve on the graph for each flap setting! What a nightmare!
I hope that helps. It's a hard concept to explain by writing and I hope you take a look at Eastlake's article above, and compare
Fig. 4 and
Fig. 5. Compare the two pictures and note where the bunched up "crowded together" streamlines appear in each case, and I think it will make sense. Hint: They're in the same spot, but one wing is upright and the other is upside down!
I'm glad to see
fish314 in this thread, and I bet
shdw would have some good insights too if he would care to weigh in. Then we can make it a total aerodynamics nerdfest.
