Page 73 - Aerodynamics for Engineering Students
P. 73

56  Aerodynamics for Engineering Students

                   direction as the local velocity vector’. Since this is identical to the condition at a
                   solid boundary it follows that:

                   (a)  any streamline may be replaced by a solid boundary without modifying the
                       flow. (This only strictly true if viscous effects are ignored.)
                   (b)  any solid boundary is itself a streamline of the flow around it.

                (ii)  A filament  (or streak) line - the line taken  up by  successive particles  of  fluid
                   passing through  some given point. A fine filament of smoke injected into the
                   flow through a nozzle traces out a filament line. The lines shown in Fig. 2.2 are
                   examples of this.
               (iii)  A path line or particle path - the path traced out by any one particle of the fluid
                   in motion.
               In unsteady flow, these three are in general different, while in steady flow all three are
               identical. Also in steady flow it is convenient to define a stream tube as an imaginary
               bundle of adjacent streamlines.




                 2.2  One-dimensional flow: the basic equations

               In all real flow situations the physical laws of conservation apply. These refer to the
               conservation  respectively of  mass,  momentum  and energy.  The equation  of  state
               completes the set that needs to be solved if some or all of the parameters controlling
               the flow are unknown.  If  a real flow can be ‘modelled’ by  a similar but  simplified
               system then  the  degree of  complexity  in handling  the  resulting  equations  may  be
               considerably reduced.
                 Historically, the lack of mathematical tools available to the engineer required that
               considerable  simplifying  assumptions  should  be  made.  The  simplifications  used
               depend on the particular problem but are not arbitrary. In fact, judgement is required
               to decide which parameters in a flow process may be reasonably ignored, at least to
               a first approximation. For example, in much  of aerodynamics the gas (air) is con-
               sidered to behave as an incompressible fluid (see Section 2.3.4),  and an even wider
               assumption is that the air flow is unaffected  by its viscosity. This last assumption
               would appear at first to be utterly inappropriate since viscosity plays an important
               role in the mechanism by which aerodynamic force is transmitted from the air flow to
               the body and vice versa. Nevertheless the science of aerodynamics progressed far on
               this assumption, and much of the aeronautical  technology  available followed from
               theories based on it.
                 Other examples will be  invoked  from time to  time and it is salutory,  and good
               engineering practice, to acknowledge those ‘simplifying’ assumptions made in order
               to arrive at an understanding of, or a solution to, a physical problem.


               2.2.1  One-dimensional flow: the basic equations
                       of conservation
               A prime simplification of the algebra involved without  any loss of physical signifi-
               cance may be made by examining the changes in the flow properties along a stream
               tube  that is essentially straight  or  for which the  cross-section  changes  slowly (i.e.
               so-called quasi-one-dimensional  flow).
   68   69   70   71   72   73   74   75   76   77   78