![]() ![]() Similar sketches can show the conditions for lift on a symmetric airfoil. It requires adjustment of the angle of attack, but as clearly demonstrated in almost every air show, it can be done. If the greater curvature on top of the wing and the Bernoulli effect are evoked to explain lift, how is this possible? The illustrations below attempt to show that an increase in airstream velocity over the top of the wing can be achieved with airfoil surface in the upright or inverted position. Part of the fascination of an aerobatics display is that with loops and upside-down flight. Illustration of different angles of attack Detractors from the Bernoulli approach often make calculations using the Kutta-Joukowski theorem (see Craig). Pragmatic difficulties exist also for those who would model the lift from Newton's third law - it is difficult to measure the downward force associated with the downwash because is is distributed in the airstream leaving the trailing edge of the airfoil. But the pragmatic success of modeling the lift with Bernoulli, neglecting density changes, suggests that the density changes are small. This does not render the Bernoulli equation invalid, it just makes it harder to apply. This is true - the ideal gas law should be obeyed and density changes will inevitably result. Those who argue against modeling the lift process with the Bernoulli equation point to the fact that the flow is not incompressible, and therefore the density changes in the air should be taken into account. Correlating the pressures with the Bernoulli equation gives reasonable agreement with observations. Such pressure measurements are typically done with Pitot tubes. Those who advocate the Bernoulli approach to lift point to detailed measurement of the pressures surrounding airfoils in wind tunnels and in flight. Conservation of angular momentum in the fluid requires an opposite circulation in the air shed from the trailing edge of the wing, and such vortex motion has been observed. Many discussions of airfoil lift invoke such a vortex in the effective circulation of air around the moving airfoil. The lift on a spinning cylinder has been clearly demonstrated, and its discussion includes a vortex in the circulating air. Those who prefer to discuss lift in these terms often invoke the Kutta-Joukowski theorem for lift on a rotating cylinder. From the conservation of momentum viewpoint, the air is given a downward component of momentum behind the airfoil, and to conserve momentum, something must be given an equal upward momentum. The fact that the air is forced downward clearly implies that there will be an upward force on the airfoil as a Newton's 3rd law reaction force. Those who advocate an approach to lift by Newton's laws appeal to the clear existance of a strong downwash behind the wing of an aircraft in flight. But perhaps it can at least indicate the lines of the discussion. This physical validity will undoubtedly not quell the debate, and this treatment will not settle it. ![]() ![]() Conservation of momentum and Newton's 3rd law are equally valid as foundation principles of nature - we do not see them violated. The Bernoulli equation is simply a statement of the principle of conservation of energy in fluids. Both are based on valid principles of physics. If the question is "Which is physically correct?" then the answer is clear - both are correct. Which is best for describing how aircraft get the needed lift to fly? Bernoulli's equation or Newton's laws and conservation of momentum? This has been an extremely active debate among those who love flying and are involved in the field. Airfoils, Bernoulli and Newton Bernoulli or Newton's Laws for Lift? ![]()
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