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264                           Distributed Model Predictive Control for Plant-Wide Systems


           on the global optimization, in which every subsystem controller has to connect with other
           subsystem controllers, which can result in high network load. The algorithm is complex and not
           convenient for engineering applications; the article in [138] improves the existing longitudinal
           multibody mass dynamic model, which optimizes the distribution of the train’s aerodynamics,
           and then designs a MPC based on the global optimization. It comes across the same problem
           as the article in [137]; since the N-DMPC with information constraints can lower the high
           network load and high calculated load caused by the global optimization, the N-DMPC is
           adopted here in the control of the high-speed train.



           12.2   System Description
           The movement of EMUs is a very complicated process, which is affected by different forces.
           The driving of EMUs considers longitudinal movement. Influence of the longitudinal move-
           ment includes traction, rolling resistance, and brake force. There are many types of EMUs
           in the cavil’s train systems, such as CRH1, CRH2, CRH3, CRH5, CRH380A, CRH380B,
           CRH380C, CRH380D, CRH6, and so on. The CRH2 is first used in the sixth time of improv-
           ing speed of the Chinese railway systems in the year 2007 when the EMUs are first used in
           Chinese dedicated passenger lines. This type has been the largest amount among the imported
           other types of EMUs.
             Different types of EMUs have different group organizations. In this chapter, we take the
           CRH2 as our research antetype.


           12.3   N-DMPC for High-Speed Trains

           12.3.1   Three Types of Force
           12.3.1.1  The Traction of EMUs
           EMUs are driven by tractions, which are generated by the electricity of the catenary [139].
           The calculation of the traction uses the method of linear interpolation by the characteristics of
           tractions for the CRH2 given in Figure 12.1.
             The traction is constrained by the adhesive force. When the force on the wheel rim is bigger
           than the adhesive force between wheels and rails, the wheel is idling. Thus, the adhesive force
           determines the upper bound of the traction.



           12.3.1.2  The Resistance of EMUs
           The resistance of EMUs includes two parts: basic resistance and additive resistance. The fric-
           tion and concussion among components, surface and air, wheels, and rails are the main reasons
           of basic resistance. The additive resistance is caused by the path.
             It is difficult to analyze the resistance theoretically because the resistance of the EMUs has
           a lot of parts. Generally, we find an approximate resistance formula for some EMUs from a
           lot of traction experiments which can be formulated by the following equation [139]:

                                        w = c + c v + c v 2                      (12.1)
                                                 1
                                                      2
                                         0
                                              0
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