Pang Y C, Reid P E, Brooks D E, Leighton K M, Bruce C
Can J Physiol Pharmacol. 1980 Sep;58(9):1078-85. doi: 10.1139/y80-162.
The uptake and distribution of halothane in dog blood were studied by analysing the whole blood and plasma concentrations of halothane in samples of arterial and mixed venous blood at different times after the induction of anesthesia with constant inspired halothane levels of 1.0, 1.5, 2.0, and 2.5%, respectively. In general a steady state was reached 2-3 h after induction. Comparison of the arterial blood concentration calculated from end-tidal halothane partial pressure with that determined by direct analysis of the blood indicated that halothane in the alveoli and halothane in arterial blood are not in thermodynamic equilibrium. The arterial halothane concentrations calculated from the end-tidal halothane partial pressure assuming equilibrium is much higher than those found experimentally; thus end-tidal halothane partial pressure is not a true measure of blood halothane concentration. The distribution of halothane between the plasma and cells in blood appeared to be sufficiently rapid to be independent of the approach to the steady state.
通过分别在吸入浓度恒定为1.0%、1.5%、2.0%和2.5%的氟烷诱导麻醉后的不同时间,分析动脉血和混合静脉血样本中氟烷的全血和血浆浓度,研究了氟烷在犬血中的摄取和分布情况。一般在诱导后2 - 3小时达到稳态。将根据呼气末氟烷分压计算出的动脉血浓度与通过直接分析血液所测定的浓度进行比较,结果表明肺泡中的氟烷与动脉血中的氟烷并非处于热力学平衡状态。假设处于平衡状态时根据呼气末氟烷分压计算出的动脉氟烷浓度远高于实验测得的浓度;因此,呼气末氟烷分压并非血液中氟烷浓度的真实度量。血液中氟烷在血浆和细胞之间的分布似乎足够迅速,与达到稳态的方式无关。