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44                          3  MODELLING AND SIMULATION OF MIXED SYSTEMS


                Table 3.1  Analogies between analogue electronics, translational and rotational mechanics
               Analogue electronics  Translational mechanics     Rotational mechanics
               Current             Force                    Torque
               i                   F                        M
               Voltage             Velocity                 Angular velocity
               u                   v                        ω
               Coil                Spring                   Torsion spring
                       d                 1  d                     1  d
               u(t) = L ·  i(t)    v(t) =  ·  F(t)          ω(t) =  ·  M(t)
                       dt                k dt                     k dt
               Capacitor           Inertia                  Rotational inertia
                      d                    d                        d
               i(t) = C  u(t)      F(t) = m  v(t)           M(t) = J  ω(t)
                     dt                   dt                       dt
               Resistor            Damping                  Rotational damping
                    1
               i(t) =  · u(t)      F(t) = b · v(t)          M(t) = b · ω(t)
                    R
                                   Mechanical power         Mechanical power
               Electrical power    dissipation due to       dissipation due to
               dissipation at resistor  damping             damping
               P(t) = u(t) · i(t)  P(t) = v(t) · F(t)       P(t) = ω(t) · M(t)
                                   Elastic energy           Elastic energy
               Magnetic energy           1 1                      1 1
                     1
                                                                        2
                       2
                                              2
               T(t) = Li (t)       T(t) =  · F (t)          T(t) =  · M (t)
                     2                   2 k                      2 k
               Electrostatic energy  Kinetic energy         Kinetic energy
                        2
                                             2
                     1
                                                                     2
                                                                  1
               T(t) = Cu (t)       T(t) =  1  mv (t)        T(t) = Jω (t)
                     2                   2                        2
               Transformer         Lever                    Gear
               i 1 · u 1 = i 2 · u 2  F 1 · v 1 = F 2 · v 2  M 1 · ω 1 = M 2 · ω 2
               i 1 = αi 2          F 1 = αF 2               M 1 = αM 2
                   1                    1                        1
               u 1 =  u 2          v 1 =  v 2               ω 1 =  ω 2
                   α                    α                        α
               Sum of all currents  Sum of all forces at a point  Sum of all moments at a point
               at a node is zero   is zero                  is zero
               Sum of all voltages in  Sum of all relative velocities  Sum of all relative angular
               a closed loop is zero  in a closed loop is zero  velocities in a closed loop is zero
               in this case, see Crandall et al. [75]. This becomes clear intuitively if we look
               at the example of a robotic arm. In the calculation of kinematics and dynamics,
               three-dimensional translational movements and triaxial rotational movements are
               calculated independently of one another. There is no parallel to this in electron-
               ics. Furthermore, analogies in the sense described are defined exclusively for the
               consideration of concentrated components and continuous quantities. Continuum
               mechanics, digital electronics and software thus remain outside their scope and
               must be considered separately.

               3.2.4    Differences between electronics and mechanics

               In what follows the primary differences between electronics and mechanics will
               once again be briefly summarized, see also Cellier [62].
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