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On Oct 16, 6:31 am, Thomas wrote:
On 9 Oct, 21:08, Le Chaud Lapin wrote: You may want to check out my web pageshttp://www.physicsmyths.org.uk/bernoulli.htm andhttp://www.physicsmyths.org.uk/drag.htm for a closer examination of the physics behind the aerodynamic lift and drag. The main point I am making there is that it is physically nonsense to claim that changing merely the tangential velocity of the air stream relative to the surface would in any way produce a resultant force (at least for a non-viscous gas). What one needs for a pressure change (and thus a force) on the surface is a change in the numbers and/or the velocity of the molecules hitting it, i.e. it is only the vertical component of the velocity that is relevant here. Only this can produce the lift for an airfoil, either because of the increased number of collisions on the lower side or the decreased number of collisions on the upper side (both situations lead to a lift). I agree, but there are some that seem to think the contrary, as you know, with the Coanda effect. http://en.wikipedia.org/wiki/Coand%C4%83_effect What is troubling about many of these theories is that, at the precise moment where the reader is most alert in anticipation of the meat of the explanation, the hand-waving begins. In the link above, the clause entitled Causes, it is written: "The effect of a spoon apparently attracting a flow of water is caused by this effect as well, since the flow of water entrains gases to flow down along the stream, and these gases are then pulled, along with the flow of water, in towards the spoon, as a result of the pressure differential. " Hmmm...."and these gases are then pulled"... pulled? By what? And it should be obvious that for this to be the case, one must either have the lower side of the wing facing to a certain degree into the airstream, and/or the upper side facing to a certain degree opposite to the airstream. This is why one either needs a certain 'angle of attack' or a correspondingly shaped airfoil. And it should be obvious that in order to have an asymmetric force (i.e. a higher upward than downward force) one needs the surfaces of the airfoil to be orientated in some way asymmetrical relatively to the airstream. So a perfectly symmetrical airfoil (front to back) at a zero angle of attack (like I indicated in Fig.1 on my pagehttp://www.physicsmyths.org.uk/bernoulli.htm) should not produce any lift as the upward force (from the rear part) is exactly equal to the downward force (from the front part). All that would happen is that the wing experiences an anti-clockwise torque. This is the reason why the rear part of the wing (behind the apex) must always have a larger surface than the front part. At least I have yet to see an airfoil where this is not the case and where it can be used at a zero angle of attack. (the Bernoulli principle is in direct contradiction to this as it would also predict a lift for a perfectly symmetric airfoil in this sense). I just read both your web pages. BTW, your explanation of d'Alembert's Paradox and the blow-over-paper- attached-to-table experiment could both use diagrams. I am trying the blow over the paper experiment now and I am not sure if I am doing it as you described. Could you provide a more vivid description so I can make sure? -Le Chaud Lapin- |
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