Page 133 - The Mechatronics Handbook
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F 1    F 2
                                                     e 1                        device
                                                  f 1
                                                                            V 1             V 2
                                                 e 2         e n
                                                       0                                   F =F = F
                                                 f 2         f n                            1  2  3
                                                 e 3                          F 1     F 2
                                                                           1       0      1
                                                    f 3
                                                                              V 1     V 2
                                                f  + f  + f  +(etc.)+ f = 0      F 3 V 3  V  − V  = V
                                                1   2  3       n                          1   2   3
                                                                         spring    1
                                               e  = e  = e = (etc.)= e                 Same velocity
                                                1  2   3        n             V spring
                                                      (a)                             (b)

                                 FIGURE 9.5  Mechanical 0-junction: (a) basic definition, (b) example use at a massless junction.



                                                                                  S      S
                                                  Effort into S  Flow into S       2      3
                                                        2            2
                                                     e            e
                                                 S      S     S      S
                                                  1  f   2     1  f   2     S                  S
                                                                             1     1     0      4
                                                    (a)           (b)                  (c)

                                 FIGURE 9.6  (a) Specifying effort from S 1  into S 2 . (b) Specifying flow from S 1  into S 2 . (c) A contrived example
                                 showing the constraint on causality assignment imposed by the physical definitions of 0- and 1-junctions.


                                 on each end is the same (note this assumes there is negligible mass). The definition of the 0-junction
                                 implies that all the bonds have different velocities, so a flow difference can be formed to construct a
                                 relative velocity, V 3 . All the bonds have the same force, however, and this force would be applied at the
                                 1-junctions that identify the three distinct velocities in this example. A spring, for example, would be
                                 connected on a bond connected to the V 3  junction, as shown in Fig. 9.5(b), and V spring  = V 3 .
                                   The 1- and 0-junction elements graphically represent algebraic structure in a model, with distinct
                                 physical attributes from compatibility of kinematics (1-junction) and force or torque (0-junction). The
                                 graph should reflect what can be understood about the interconnection of physical devices with a bond
                                 graph. There is an advantage in forming a bond graph, since causality can then be used to form
                                 mathematical models. See the text by Karnopp, Margolis, and Rosenberg [17] for examples. There is a
                                 relation to through and across variables, which are used in linear graph methods [33].


                                 Causality
                                 Bond graph modeling was conceived with a consistent and algorithmic methodology for assignment of
                                 causality (see Paynter [28], p. 126). In the context of bond graph modeling, causality refers to the input–
                                 output relationship between variables on a power bond, and it depends on the systems connected to
                                 each end of a bond. Paynter identified the need for this concept having been extensively involved in
                                 analog computing, where solutions rely on well-defined relationships between signals. For example, if
                                 system S 1  in Fig. 9.6(a) is a known source of effort, then when connected to a system S 2 , it must specify
                                 effort into S 2 , and S 2  in turn must return the flow variable, f, on the bond that connects the two systems.
                                 In a bond graph, this causal relationship is indicated by a vertical stroke drawn on the bond, as shown
                                 in Fig. 9.6(a). The vertical stroke at one end of a bond indicates that effort is specified into the multiport
                                 element connected at that end. In Fig. 9.6(b), the causality is reversed from that shown in (a).

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