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334    Chapter 11



                                                100
                                              V (L/min)  50                                       50% End Flow


                                                                          5 L/min End Flow


                                                            1       2        3       4       5        6       7





                                              P (cm H 2 O)  2100                                Increased End Flow




                                                 40                     Increased End Flow      Increased End P TA
                                                                        Increased End P
                                                                                     TA

                                                                  P ALV                     P ALV

                                                22          1       2       3        4       5       6        7  © Cengage Learning 2014

                                                                            Time (sec)
                                            Figure 11-16  Effects of end flow on the pressure waveforms during descending ramp flow 
                                            ventilation. Figure shows two end flows: 5 L/min (left) and 50% of peak inspiratory flow (right). 
                                            Increase of end flow raises the transairway pressure (P TA ), but not the alveolar pressure (P ALV ).


                                            Effects of End-Flow on End-Transairway Pressure


                                            Figure 11-16 demonstrates the changes in P  patterns that could be expected
                                                                                   TA
                          (Figure 11-16) During   when end-flows for DRFWs are increased. In the first example, the end-flow is
                        descending ramp flow ventila-
                        tion, a higher end-flow raises   5 L/min (PB840). The pressure pattern shows a slight increase in the P  above
                                                                                                          TA
                        the P TA  at end-inspiratory, but   the P   at the end of inspiration as a result of the slight resistance to end-flow
                        not the alveolar pressure (P ALV ).  ALV
                                            being above baseline. The second set of waveforms shows a 50% DRFW where
                                            end-flow is 50% of the initial peak flow set. The initial flow set is very high
                                            (100 L/min), which causes an exponential rise in initial P  (40 cm H O) because
                                                                                                       2
                                                                                             TA
                                            of turbulent flow and circuit/airway resistance. The end-P  is also relatively high
                                                                                             TA
                                            from resistance to flow above the peak P ALV  compared to the first example since
                                            end-flow is 50 L/min (50% of 100 L/min) compared to 5 L/min. These flow and
                                            pressure patterns do not represent ventilation of the same patient. Peak P ALV  is
                                            at the same level, but V  delivered is much greater for the second flow waveform
                                                                T
                                            example compared to the first.

                                            Distribution of Delivered Tidal Volume


                                            In Figure 11-17, volume-time waveforms have been added for comparison with
                                            DRFW and pressure-time waveforms. Since flow rate is highest in the beginning
                                            of inspiration for a DRFW, the slope in rise to peak volume, like P ALV , is initially






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