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The two examples in Figs. 9.20(b) and 9.20(c) demonstrate how a relative velocity can be formed. Two
                                 masses each identify the two distinct velocity points in these systems. Using a 0-junction allows con-
                                 struction of a velocity difference, and in each case this forms a relative velocity. In each case the relative
                                 velocity is represented by a 1-junction, and it is critical to identify that this 1-junction is essentially an
                                 attachment point for a basic mechanical modeling element.


                                 Assigning and Using Causality
                                 Bond graphs describe how modeling decisions have been made, and how model elements (R, C, etc.)
                                 are interconnected. A power bond represents power flow, and assigning power convention using a half-
                                 arrow is an essential part of making the graph useful for modeling. A sign convention is essential for
                                 expressing the algebraic summation of effort and flow variables at 0- and 1-junctions. Power is generally
                                 assigned positive sense flowing into passive elements (resistive, capacitive, inertive), and it is usually safe
                                 to always adopt this convention. Sign convention requires consistent and careful consideration of the
                                 reference conditions, and sometimes there may be some arbitrariness, not unlike the definition of
                                 reference directions in a free-body diagram.
                                   Causality involves an augmentation of the bond graph, but is strictly independent of power  flow
                                 convention. As discussed earlier, an assignment is made on each bond that indicates the input–output
                                 relationship of the effort-flow variables. The assignment of causality follows a very consistent set of rules.
                                 A system model that has been successfully assigned causality on all bonds essentially communicates
                                 solvability of the underlying mathematical equations. To understand where this comes from, we can
                                 begin by examining the contents of Tables 9.4 and 9.5. These tables refer to the integral form of the energy
                                 storage elements. An energy storage element is in integral form if it has been assigned integral causality.
                                 Integral causality implies that the causal input variable (effort or flow) leads to a condition in which the
                                 state of the energy stored in that element can be determined only by integrating the fundamental rate
                                 law. As shown in Table 9.7, integral causality for an I element implies effort is the input, whereas integral
                                 causality for the C element implies flow is the input.

                                    TABLE 9.7  Table Summarizing Causality for Energy Storage Elements
                                                Integral Causality                   Derivative Causality

                                             e          CONSTITUTIVE                e         INVERSE
                                      C                 e =ΦC (q)            C                CONSTITUTIVE
                                                                                                  −1
                                           f = q                                  f = q       q =ΦC (e)
                                                                                  −1
                                         ΦC ( )    e    f                        ΦC ()        q
                                                                                         e
                                      q                                      q
                                                            q(t)                  d                    f = dq/dt
                                         ∫ ()dt                                   dt
                                                  f                                       f              t
                                                             q(t)   t
                                                                       dt
                                                                                              INVERSE
                                           e = p       CONSTITUTIVE               e = p       CONSTITUTIVE
                                      I                 f =ΦI (p)            I                    −1
                                            f                                       f         p =ΦI (f )
                                                                                  d                      dp/dt
                                         ∫ ()dt         e                                     p       e=
                                                   e                              dt     e
                                       p                     p(t)             p

                                                                                  −1
                                         ΦI ()                                   ΦI ()
                                                  f                                      f
                                                                    t                                    t

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