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Potential flow

































                 3.1  Introduction

               The concept of irrotational flow is introduced briefly in Section 2.7.6. By definition
               the vorticity is everywhere zero for such flows. This does not immediately seem a very
               significant simplification. But it turns out that zero vorticity implies the existence of a
               potential  field (analogous to gravitational and electric fields). In aerodynamics the
               main variable of the potential field is known as the velocity potential (it is analogous
               to voltage in electric fields). And another name for irrotational flow is potentialflow.
               For such flows the equations of motion reduce to a single partial differential equa-
               tion,  the  famous  Laplace  equation,  for  velocity  potential.  There  are  well-known
               techniques (see Sections 3.3 and  3.4) for  finding analytical  solutions  to  Laplace’s
               equation that can be applied to aerodynamics. These analytical techniques can also
               be  used  to  develop  sophisticated  computational  methods  that  can  calculate  the
               potential flows around the complex three-dimensional geometries typical of modern
               aircraft (see Section 3.5).
                 In Section 2.7.6 it was explained that the existence of vorticity is associated with
               the  effects of  viscosity.  It  therefore  follows  that  approximating  a  real  flow  by  a
               potential flow is tantamount to ignoring viscous effects. Accordingly, since all real
               fluids are viscous, it is natural to ask whether there  is  any practical  advantage  in
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