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216                6. NEURAL NETWORK SEMIEMPIRICAL MODELING OF AIRCRAFT MOTION

                         acterize the total effect that the errors of these  practical due to the difficulties encountered in
                         function approximations have on the accuracy  obtaining the informative data set required to
                         of the trajectory predictions given by the model.  find the axial force coefficient C x . For this reason,
                         These results can be regarded as completely sat-  the overall problem of aerodynamic character-
                         isfactory. However, it is also of interest to an-  istics identification has been divided into two
                         alyze how accurately the problem of the aero-  subproblems. The first subproblem, considered
                         dynamic characteristics identification has been
                                                                      in Section 6.3, is the problem of identification
                         solved.
                                                                      of the five coefficients C y , C z , C l , C n , C m in the
                            To answer this question, we need to extract
                                                                      case of three-axis rotational motion. The second
                         the ANN modules corresponding to the approx-
                                                                      subproblem, considered in this section, amounts
                         imated functions C y , C z , C l , C n , C m and then
                                                                      to the identification of the remaining axial force
                         compare the values they yield with the avail-
                                                                      coefficient C x in the case of longitudinal motion
                         able experimental data [20]. Integral estimates of
                                                                      (both translational and angular). In addition, in
                         the accuracy can be obtained, for example, with
                         the RMSE function. In the experiments above we  [3,4], in order to reduce the computational com-
                                                                      plexity of the problem being solved, the solution
                                                                  =
                         have the following error estimates: RMSE C y
                         5.4257 · 10 −4  ,RMSE C z  = 9.2759 · 10 −4  , RMSE C l  =  of the modeling and identification problem was
                         2.1496·10 −5 ,RMSE C m  = 1.4952·10 −4  , RMSE C n  =  not carried out for the full range of possible val-
                         1.3873 · 10 −5 . The values of the reproduction er-  ues of the state variables and the controls for
                         ror for the functions C y , C z , C l , C n , C m for each  the dynamical system under consideration, but
                         time instant during the testing of the semiempir-  only for its part (on the order of several percent
                         ical model are shown in Fig. 6.10.           of the range of values of each of the variables).
                                                                      In this section, we extract the dependencies for
                                                                      the coefficients C x , C z , C m on a radically more
                         6.4 SEMIEMPIRICAL MODELING OF                wide range of possible values of their arguments
                                       LONGITUDINAL                   (for the list of these arguments, see (6.11)and
                                   TRANSLATIONAL AND                  (6.12)).
                                 ANGULAR MOTION FOR A                    The identification problem for the axial aero-
                                                                                    ¯
                                                                      dynamic force X as a nonlinear function of the
                                MANEUVERABLE AIRCRAFT
                                                                      corresponding arguments is traditionally chal-
                                                                      lenging to solve (see, for example, [32,33]). Sim-
                            In this section, we consider the problem of the  ilarly, the problem of finding the aircraft engine
                         longitudinal motion modeling for a maneuver-  thrust F T value is difficult [32,33]. We need this
                         able aircraft as well as the identification prob-  value to extract X from the total force R X mea-
                                                                                     ¯
                         lem for its aerodynamic characteristics, such as
                                                                      sured during the flight experiment. The ANN
                         the coefficients of aerodynamic axial and nor-
                         mal forces, and the pitching moment. We solve  modeling methods seem to be a promising tool
                                                                      for the solution of this problem in the same
                         this problem in the same way as the problems
                         in the previous two sections, by using a class  way as it was for the other aerodynamic char-
                         of semiempirical dynamic models that combine  acteristics identification. This hypothesis is sup-
                         the possibilities of theoretical and neural net-  ported by the theoretical results (see, for exam-
                         work modeling.                               ple, [34–36]), which show that an artificial neural
                            In Section 6.3, it was shown that the simul-  network has the properties of a universal ap-
                         taneous reconstruction of the dependencies for  proximator, i.e., it can represent any mapping of
                         all six aerodynamic forces and moments is im-  an n-dimensional input into an m-dimensional
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