Page 38 - Aerodynamics for Engineering Students
P. 38

Basic concepts and definitions  21

              Rearranging Eqn (1.36), it becomes


                                                  V  Vd  -f
                                         n= c Cd (7)                             (1.37)
              or, alternatively,


                                           ($) =g(?)                             (1.38)


              where g represents some function which, as it includes the undetermined constant C
              and index f, is unknown from the present analysis.
                Although it may not appear so at first sight, Eqn (1.38) is extremely valuable, as it
              shows that the values of nd/V should depend only on the corresponding value of
              Vd/v, regardless of the actual values of the original variables. This means that if, for
              each observation, the values of nd/V and Vd/v are calculated and plotted as a graph,
              all  the  results should  lie on  a  single curve, this  curve representing the  unknown
              function g. A person wishing to estimate the eddy frequency for some given cylinder,
              fluid  and  speed need  only  calculate the  value  of  Vd/v, read  from  the  curve the
              corresponding value of nd/V and convert this to eddy frequency n. Thus the results
              of the series of observations are now in a usable form.
                Consider for a moment the two compound variables derived above:
              (a)  nd/V. The dimensions of this are given by
                                nd                -1  -1
                                -=  [T-I  x L x (LT   )  ] = [LOTo] = [l]
                                V
              (b)  Vd/v. The dimensions of this are given by

                                  Vd
                                  - [(LT-') x L x (L2T-')-']  = [l]
                                     =
                                   v
                Thus the above analysis has collapsed the five original variables n, d, V, p and v
              into two  compound  variables, both  of  which  are non-dimensional. This has  two
              advantages: (i) that the values obtained for these two quantities are independent of
              the consistent system of units used; and (ii) that the influence of four variables on a
              fifth term can be shown on a single graph instead of an extensive range of graphs.
                It can now be seen why the index  f was left unresolved. The variables with indices
              that were resolved appear in both dimensionless groups, although in the group nd/ V
              the density p is to the power zero. These repeated variables have been combined in
              turn with each of the other variables to form dimensionless groups.
                There are certain problems, e.g. the frequency of vibration of a stretched string, in
              which all the indices may be determined, leaving only the constant C undetermined.
              It is, however, usual to have more indices than equations, requiring one index or
              more to be left undetermined as above.
                It must be noted that, while dimensional analysis will show which factors are not
              relevant to a given problem, the method cannot indicate which relevant factors, if
              any, have been left out. It is, therefore, advisable to include all factors likely to have
              any bearing on a given problem, leaving out only those factors which, on a priori
              considerations, can be shown to have little or no relevance.
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