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PHYSICAL AND FLOW PROPERTIES OF BLOOD  91











                                FIGURE 3.18  Lumped-parameter electrical model of a multicompartment arterial segment.

                          For a system of vessels attached in series (or small units of a nonuniform vessel) a more complicated
                          scheme, composed of a series of compartments whose characteristics are represented by R , C , and
                                                                                           i
                                                                                              i
                          L (Fig. 3.18), is used. For this case, Kirchhoff’s law applied to each loop will yield
                           i
                                                                    dQ
                                                     P −  P i−1  =  R Q +  L i               (3.50)
                                                      i
                                                               i
                                                              i
                                                                    dt
                                                              V
                                                           P =  i                            (3.51)
                                                            i
                                                              C
                                                               i
                                                                 dV
                                                        Q −  Q i−1  =  i                     (3.52)
                                                         i
                                                                 dt
                          The problem is reduced to a set of linear differential equations and can be solved for given bound-
                          ary conditions. The RCL characteristics of a given problem may be derived from the known physi-
                          cal properties of blood and blood vessels (Dinnar, 1981; Van der Twell, 1957). This compartmental
                          approach allowed for computer simulations of complex arterial circuits with clinical applications
                          (McMahon et al., 1971; Clark et al., 1980; Barnea et al., 1990; Olansen et al., 2000; Westerhof and
                          Stergiopulos, 2000; Ripplinger et al., 2001).
              ACKNOWLEDGMENT
                          The authors are thankful to Dr. Uri Zaretsky for his technical assistance.

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