Turner J C
Department of Chemical Engineering, University of Exeter, England.
J Clin Monit. 1991 Jul;7(3):237-40. doi: 10.1007/BF01619266.
Anesthetic gases from several patients can be monitored simultaneously with a centrally located mass spectrometer. Such monitoring requires catheters from patient to spectrometer that are several meters long. Scamman (J Clin Monit 1988; 4:227-229) found that when the respiratory frequency is high, as with infants, the CO2 signal from the patient is unacceptably distorted during passage down the catheter. This is due to Taylor dispersion of the input signal. An outline of the theory of Taylor dispersion is given. The equations describe the interaction between the velocity distribution (which, in laminar flow, is parabolic) and the radial diffusion of CO2. This interaction keeps a tracer signal together in a pulse, as it moves down the tube with the mean velocity, spreading somewhat as it proceeds. How much does an initially sharp signal become blurred? The spread of such a signal when it reaches the detector, measured in time, can be expressed in various ways. Measurement is complicated, however, by the fact that the gas pressure may fall by as much as a factor of 10 along the line. The resultant expansion and acceleration of the gas cannot be ignored. A full treatment of this complication is given elsewhere, but the following simple equation is described: delta t = 3.54 x 10(-3) l [(1 + R2)/(1 - R2)]1/2. Typically, the spread time is up to a quarter of a second for catheters of 50 m, such as used by Scamman. This is comparable with the period of CO2 rise and fall for infants and explains the serious distortion in wave form that Scamman+ found.(ABSTRACT TRUNCATED AT 250 WORDS)
来自多名患者的麻醉气体可通过位于中央的质谱仪同时进行监测。这种监测需要从患者到质谱仪的长达数米的导管。斯卡曼(《临床监测杂志》1988年;4:227 - 229)发现,当呼吸频率较高时,如婴儿,患者的二氧化碳信号在沿导管传输过程中会出现不可接受的失真。这是由于输入信号的泰勒扩散。文中给出了泰勒扩散理论的概述。这些方程描述了速度分布(在层流中为抛物线形)与二氧化碳的径向扩散之间的相互作用。这种相互作用使示踪信号在随平均速度沿管道移动时保持在一个脉冲内,并在前进过程中有所扩散。最初尖锐的信号会变得多模糊呢?当信号到达探测器时,以时间衡量的这种信号扩散可以用多种方式表示。然而,由于气体压力沿线可能下降多达10倍这一事实,测量变得复杂。气体的由此产生的膨胀和加速不能被忽略。对此并发症的全面处理在其他地方给出,但描述了以下简单方程:δt = 3.54 x 10(-3) l [(1 + R2)/(1 - R2)]1/2。对于斯卡曼使用的50米长的导管,典型的扩散时间长达四分之一秒。这与婴儿二氧化碳上升和下降的周期相当,解释了斯卡曼发现的严重波形失真。(摘要截短于250字)