Subtitles section Play video Print subtitles There is an intriguing phenomenon when you closely examine the science behind airfoils. Why does the air above the airfoil flow much faster than the air below? How come the two never meet? The answer is right there in the pressure gradient. Before explaining the reason, we will first describe how the pressure gradient is developed. In the first part of the airfoil video we learned that the flow gets curved as shown to the kiwanda effect. You can explain the pressure distribution by keeping in mind that in a curved flow pressure is higher at the outside. There are three main flow curvatures in this flow. The biggest is at the top of the airfoil. Far away from the airfoil the pressure is atmospheric so due to this high curvature pressure will decrease as we move toward the airfoil. The second curvature is at the bottom of the airfoil near the tail, this is also curved downward so here if we move toward the airfoil, the pressure should increase. The last flow curvature is also at the bottom of the airfoil close to the leading edge. This is a very small curvature this curvature, however, is curved slightly upward. This means that the pressure should decrease in this region as we move toward the airfoil. Due to the very small curvature there will be a very small drop in pressure. We know that far away from the upstream and downstream the pressure is atmospheric. At the leading edge of the airfoil, a high-pressure region is generated as the flow directly hits this portion so we can easily construct the pressure distribution as shown The CFD results could form exactly two are logical conclusions. Now back to the initial question to facilitate the analysis we can neglect this very small drop in pressure. You can see that at the top the pressure decreases almost to the midpoint before it increases at the bottom the pressure keeps on increasing until it reaches the tail only after that does it decrease. Pause for a moment now and consider two fluid particles starting at the same speed but in different pressure gradients. The top particle is surrounded by a decreasing pressure condition while the bottom particle sits in an increasing pressure condition. For the top particle pressure on the right side is less than at the left side so there will be a net force in the same direction of the velocity and the particle will speed up. However, the reverse is true for the bottom particle here the net forces against velocity direction so it will decelerate. In short, in a decreasing pressure filled the fluid particle will accelerate and in an increasing pressure filled the fluid particle will decelerate. This is exactly what happens in an airfoil also the bottom particle will keep on decelerating the top particle will accelerate up to the midpoint. This means that the speed of the top particle will be higher at any point in time and the two particles will never meet. The bottom particle also experiences of pressure decreasing scenario, However, it is almost after the trailing edge and it happened suddenly such a sudden drop in pressure will not considerably increase the particle speed. In short for this particular problem the pressure distribution makes the particles flow at different speeds but the reverse argument does not hold the different speeds of the particles are not what make the pressure distribution because for the second textbook argument there is no logical explanation for what causes this speed difference? These two arguments are not too different ways of looking at the same thing. Support us so that we can continue creating engineering videos for you please help us at patreon.com thank you.
B1 US pressure particle curvature flow curved bottom Why is the top flow faster over an Airfoil ? 25 4 Sam Cheng posted on 2017/04/14 More Share Save Report Video vocabulary