Page 78 - Modern Control Systems
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52               Chapter 2  Mathematical  Models of  Systems

                           linear, dynamic elements  is given in Table 2.2  [5]. The equations in Table 2.2 are  ideal-
                           ized  descriptions  and  only  approximate  the  actual  conditions  (for  example, when  a
                           linear, lumped  approximation  is used  for  a distributed  element).




           Table 2.2  Summary of Governing Differential Equations for Ideal Elements

           Type of            Physical              Governing      Energy £ or
           Element            Element               Equation       Power  SP      Symbol
                                                         _ di
                           (  Electrical  inductance               E  =  i-Li 2
                                                                       2
                                                         J.  dF_
                              Translational  spring  «21  =        E
                                                         k  dt      ~  2  k
           Inductive storage  <
                              Rotational  spring         1  dT         III
                                                    <»2\ = =  - —  E  =
                                                         k  dt         2  k
                                                          dQ
                              Fluid  inertia                       E  =  - 21<?
                                                          dt
                              Electrical  capacitance    dv 2i                         i  \\C
                                                    i  =  C               y 2 i   v 2  o—*—    o  vi
                                                         dt
                              Translational  mass   F  =  M  dv 2   E  =  -Mv 2 2  '-sH^Hl-
                                                          dt           2              v 2
                                                                                            constant
           Capacitive storage  ^  Rotational  mass  T  =  J  da) 2                            to,  =
                                                          dt                                constant
                                                          dP 2i
                              Fluid  capacitance    Q  =  C f      E  =  -C fP^
                                                           dt
                            <  Thermal  capacitance    rdV 2       E  = C<5 2
                                                                                     9" 2    9",  -
                                                                                           constant
                                                                                             i
                                                                                        R
                           (  Electrical resistance   i =  ±va            n       v 2 o— V\A/—*-°  v \
                                                                                       /
                                                                       R
                              Translational  damper  F  =  bv '21   9»  =  bv 2i 2
                                                                                      v 2
           Energy dissipators  <  Rotational  damper  T  =  bco 21   9»  =  ba) 21 2
                                                                                  T—K>    1 I  OG>I
                                                                                      G>2  —>b
                                                                   9      p
                              Fluid  resistance     Q                 = i »             R f  Q
                                                      = ¥/-                       P 2 o-AAA/  >  ° f |

                              Thermal  resistance   d =  J**       9  =  ^ ¾            R t  q
                                                                                  °T 2 o-^VVV  >  o3"i
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