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144  Aerodynamics for Engineering Students

                    From Eqns (3.77) and (3.78b) it follows that the velocity on the surface of the
                  sphere is given by

                                                    3
                                                q = - Usinp
                                                    2
                  So that using the Bernoulli equation gives that
                                            1          1
                                       Po + 2 PU2 = p + pp"





                  Therefore the pressure variation over the sphere's surface is given by
                                                   1       9
                                          p-po =-u2(1 --sin2p)                       (3.81)
                                                   2       4
                  Again this result is quite similar to that for the circular cylinder described in Section
                  3.3.9 and depicted in Fig. 3.23.

                  3.4.6  Flow around slender bodies

                  In the foregoing part of this section it has been shown that the flow around a class of
                  bodies  of  revolution can  be  modelled by  the  use  of  a  source and  sink  of  equal
                  strength. Accordingly, it would be  natural to speculate whether the  flow  around
                  more general body shapes could be obtained by using several sources and sinks or a
                  distribution of them along the z axis. It is indeed possible to do this as first shown by
                  Fuhrmann.* Two examples similar to those presented by him are shown in Fig. 3.31.
                  Although Fuhrmann's method could model the flow around realistic-looking bodies
                  it suffered an important defect from the design point of view. One could calculate the
                  body of revolution corresponding to a specified distribution of sources and sinks, but a
                  designer would wish to be able to solve the inverse problem of how to choose the variation
                  of source strength in order to obtain the flow around a given shape. This more practical
                  approach became possible after Munkt introduced his slender-body theory for calculat-
                  ing the forces on airship hulls. A brief description of this approach is given below.













                  Fig. 3.31  Two examples of flow around bodies of  revolution generated by (a) a point source plus a linear
                  distribution  of  source strength; and (b) two linear distributions  of source strength. The source distributions
                  are denoted by broken lines

                  * Fuhrmann, G. (191 l), Drag and pressure measurements on balloon models (in German), 2. &tech.,   11, 165.
                   Munk, M.M. (1924),  The Aerodynamic Forces on Airship Hulls, NACA Report 184.
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