Page 323 - Mechanical Engineers' Handbook (Volume 2)
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314   Mathematical Models of Dynamic Physical Systems

                          applies to any closed path in the system. For convenience and to ensure the independence
                          of the resulting equations, continuity is usually applied to the meshes or ‘‘windows’’ of the
                          graph. A one-part graph with n nodes and b branches will have b   n   1 meshes, each
                          mesh yielding one independent compatibility equation. A planar graph with p separate parts
                          (resulting from multiport elements) will have b   n   p independent compatibility equations.
                          For a closed path q, the compatibility equation is

                                                            v   0
                                                          q  ij
                          where the summation is taken over all branches (i, j) on the path.
                             For the system graph depicted in Fig. 6b, the three compatibility equations based on
                          the meshes are

                                           path 1 → 2 → g → 1:   v   v m 2    v m 1    0
                                                                  b
                                           path 1 → 2 → 1:            v   v   0
                                                                        k 1  b
                                           path 2 → 3 → g → 2:   v   v   v      0
                                                                   k 2  s  m 2
                          These equations are all mutually independent and express apparent geometric identities. The
                          first equation, for example, states that the velocity difference between the ends of the damper
                          is identically the difference between the velocities of the masses it connects. Compatibility
                          relations are also known as path, loop, and connectedness relations.


           3.4  Analogs and Duals
                          Taken together, the element laws and system relations are a complete mathematical model
                          of a system. When expressed in terms of generalized through and across variables, the model
                          applies not only to the physical system for which it was derived, but also to any physical
                          system with the same generalized system graph. Different physical systems with the same
                          generalized model are called analogs. The mechanical rotational, electrical, and fluid analogs
                          of the mechanical translational system of Fig. 6a are shown in Fig. 7. Note that because the
                          original system contains an inductive storage element, there is no thermal analog.
                             Systems of the same physical type but in which the roles of the through variables and
                          the across variables have been interchanged are called duals. The analog of a dual—or,
                          equivalently, the dual of an analog—is sometimes called a dualog. The concepts of analogy
                          and duality can be exploited in many different ways.




           4  STANDARD FORMS FOR LINEAR MODELS
                          The element laws and system relations together constitute a complete mathematical descrip-
                          tion of a physical system. For a system graph with n nodes, b branches, and s sources, there
                          will be b   s element laws, n   1 continuity equations, and b   n   1 compatibility
                          equations. This is a total of 2b   s differential and algebraic equations. For systems com-
                          posed entirely of linear elements, it is always possible to reduce these 2b   s equations to
                          either of two standard forms. The input/output, or I/O, form is the basis for transform or
                          so-called classical linear systems analysis. The state-variable form is the basis for state-
                          variable or so-called modern linear systems analysis.
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