TY - JOUR
T1 - Effects of mean airway pressure on gas transport during high-frequency ventilation in dogs
AU - Yamada, Y.
AU - Venegas, J. G.
AU - Strieder, D. J.
AU - Hales, C. A.
PY - 1986
Y1 - 1986
N2 - In 10 anesthetized, paralyzed, supine dogs, arterial blood gases and CO2 production (V̇CO2) were measured after 10-min runs of high-frequency ventilation (HFV) at three levels of mean airway pressure (P̄aw) (0, 5, and 10 cmH2O). HFV was delivered at frequencies (f) of 3, 6, and 9 Hz with a ventilator that generated known tidal volumes (VT) independent of respiratory system impedance. At each f, VT was adjusted at P̄aw of 0 cmH2O to obtain a eucapnia. As P̄aw was increased to 5 and 10 cmH2O, arterial PCO2 (Pa(CO2)) increased and arterial PO2 (Pa(O2)) decreased monotonically and significantly. The effect of P̄aw on Pa(CO2) and Pa(O2) was the same at 3, 6, and 9 Hz. Alveolar ventilation (V̇A), calculated from V̇CO2 and Pa(CO2), significantly decreased by 22.7 ± 2.6 and 40.1 ± 2.6% after P̄aw was increased to 5 and 10 cmH2O, respectively. By taking into account the changes in anatomic dead space (VD) with lung volume, V̇A at different levels of P̄aw fits the gas transport relationship for HFV derived previously: V̇A = 0.13 (VT/VD)1.2VTf (J. Appl. Physiol. 60: 1025-1030, 1986). We conclude that increasing P̄aw and lung volume significantly decreases gas transport during HFV and that this effect is due to the concomitant increase of the volume of conducting airways.
AB - In 10 anesthetized, paralyzed, supine dogs, arterial blood gases and CO2 production (V̇CO2) were measured after 10-min runs of high-frequency ventilation (HFV) at three levels of mean airway pressure (P̄aw) (0, 5, and 10 cmH2O). HFV was delivered at frequencies (f) of 3, 6, and 9 Hz with a ventilator that generated known tidal volumes (VT) independent of respiratory system impedance. At each f, VT was adjusted at P̄aw of 0 cmH2O to obtain a eucapnia. As P̄aw was increased to 5 and 10 cmH2O, arterial PCO2 (Pa(CO2)) increased and arterial PO2 (Pa(O2)) decreased monotonically and significantly. The effect of P̄aw on Pa(CO2) and Pa(O2) was the same at 3, 6, and 9 Hz. Alveolar ventilation (V̇A), calculated from V̇CO2 and Pa(CO2), significantly decreased by 22.7 ± 2.6 and 40.1 ± 2.6% after P̄aw was increased to 5 and 10 cmH2O, respectively. By taking into account the changes in anatomic dead space (VD) with lung volume, V̇A at different levels of P̄aw fits the gas transport relationship for HFV derived previously: V̇A = 0.13 (VT/VD)1.2VTf (J. Appl. Physiol. 60: 1025-1030, 1986). We conclude that increasing P̄aw and lung volume significantly decreases gas transport during HFV and that this effect is due to the concomitant increase of the volume of conducting airways.
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U2 - 10.1152/jappl.1986.61.5.1896
DO - 10.1152/jappl.1986.61.5.1896
M3 - Article
C2 - 3096948
AN - SCOPUS:0022971567
SN - 8750-7587
VL - 61
SP - 1896
EP - 1902
JO - Journal of Applied Physiology Respiratory Environmental and Exercise Physiology
JF - Journal of Applied Physiology Respiratory Environmental and Exercise Physiology
IS - 5
ER -