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62    Computational Modeling in Biomedical Engineering and Medical Physics


                proportional to the group K B t 1=2 = t 1 1 t 2 Þ. The metabolic rate of the animal
                                                   ð
                emerges as a constraint, as in Eq. (2.21)
                                              1=2
                                             t
                                              2   BK constantÞ:
                                            t 1 1 t 2  ð                              ð2:25Þ
                   The power consumption of the heart is then proportional to the inverse of
                        1=2                 _
                t 2 1 2 Kt  . It follows that W-N for t 2 - 0; K 2 2f  g, and at the intermediate
                                  22
                value t 2;opt B 4=9 K  it exhibits a relatively sharp minimum. The constraint K on

                the mass transfer provides the contraction time t 1;opt B 2=9 K 22 . Interesting enough
                (Bejan, 2000a,b)
                                                   21=2
                                                AD     ΔC
                                          22
                                t 1 ; t 2 Þ BK  5           ; t 1;opt =t 2;opt B1=2;
                                                     _ m
                               ð    opt                                               ð2:26Þ
                whichare valid for animalsinawide rangeofsizes (Peters, 1983; Schmidt-Nielsen, 1984).
                   It may be inferred the existence of an eigen frequency of the heartbeats that mini-
                mizes the mechanical power consumed by the heart, subject to the constraints of the
                interface and the mass transfer, or metabolic rate of O 2 . This maximization with
                respect to the active diffusion time interval is the foundation of all optimal pulsations
                in the engineered and natural systems.


                Coupled rhythms in the cardio-pulmonary system
                Within the framework of the thermodynamics with finite speed (TFS), the cardio-
                pulmonary system (CPS), may be considered as an ensemble of two biological machines,
                naturally designed and optimized: the heart, a “naturally designed” blood (liquid) pump,
                and the lungs, “naturally designed” air compressors (Petrescu et al., 2018). Studies based
                on a large number of measurements, for stationary states related to different positions:
                walking, sitting, laying, repetitive exercise, etc., have shown that the two frequencies—
                for heart, f H , and lung, f L —are correlated, for a healthy person, through

                                             f H 5 f L 2 1 N=4 :                      ð2:27Þ

                   Here N is an integer, called quantum number of the interaction between the heart and
                lung in a stationary state. It is thought of as the interaction parameter that links the
                two biological machines (heart and lungs), namely the difference in phase between
                them (Petrescu et al., 2018). The analogy with classical thermodynamics indicates that
                Eq. (2.27) relates three state parameters (f H , f L , N), of which obviously only two may
                be independent. Three particular processes are then identified: (1) iso-pulse
                (f H 5 const.); (2) iso-rhythm (f L 5 const.); and (3) iso-quantum (N 5 const.). Moreover, it
                has been observed that CPS works properly (healthy) only if certain coordination in
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