Page 35 - Understanding Flight
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CH02_Anderson  7/25/01  8:55 AM  Page 22




                 22  CHAPTER TWO




                    On May 9, 1926, Commander R.E.  means that the volume of a mass of air remains constant and
                    Byrd made the first flight over  that flows of air do not separate from each other to form voids
                    the North Pole. On Nov. 28–29,  (gaps). For the moment let us consider the Coanda effect with
                    1929, Byrd made the first flight  water. This effect can be demonstrated in a simple way. Run a
                    over the South Pole.      small stream of water from a faucet and bring a horizontal
                                              water glass over to it until it just touches the water, as in Fig-
                                       ure 2.4. As in the figure, the water will wrap partway around the glass.
                                       From Newton’s first law we know that for the flow of water to bend
                                       there must be a force on it. The force is in the direction of the bend.
                                       From Newton’s third law we know that there must be an equal and
                                       opposite force acting on the glass. The same phenomenon causes
                                       forces between the airflow around a wing and the wing. So why do
                                       fluids tend to bend around a solid object?
                                         The answer is viscosity, that characteristic that makes a fluid thick
                                       and makes it stick to a surface. When a moving fluid comes into
                                       contact with a solid object, some of it sticks to the surface. A small
                                       distance from the surface the fluid has a small velocity with respect
                                       to the object. As in Figure 2.5, the farther one looks from the surface,
                                       the faster the fluid is flowing, until it eventually comes to the speed
                                       of the uniform flow some distance away from the object. The
                                       transition layer between the surface and the fluid at the uniform flow
                                       is called the boundary layer, which is discussed in the next chapter.












                                               Force on glass




                                                                    Force on water




                                       Fig. 2.4. The Coanda effect.
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