Naitoh Y, Shirato M
Nihon Jibiinkoka Gakkai Kaiho. 1989 Nov;92(11):1884-94. doi: 10.3950/jibiinkoka.92.1884.
The nasal patency during respiration is today usually expressed by the nasal resistance. However, the nasal resistance is not the same throughout the total respiratory phase. Therefore, the reference point to express the resistance is therefore necessary to facilitate the mutual comparison of the data. The international committee for standardization of rhinomanometry has been paying a great effort to decide where this reference point should be set up, but has not yet reached the final consensus. The purpose of this study is to present a new method to estimate nasal respiratory conductivity, regardless of the reference point. Pressure flow curves during nasal respiration are quite similar in nature and rarely cross one another. The parabolic curves which do not cross each other can be superimposed by multiplying the standard equation, V = n.f(P). Accordingly, n is only one parameter in comparing these curves. A standard curve is decided as follows. Rohrer's equation was examined by polynomial regression analysis and concluded to be adequate to simulate a pressure flow curve. Rohrer's equation is converted to the function of P. Integration of this equation along P gives the value of the area under the curve (AUC). The total AUC can be obtained by simply adding the AUC of right and left sides. Definite integration from the origin to 1.0 and 2.0 on the abscissa gives the numerical value of AUC in each curve. The mean AUC is easily calculated by simple mathematical averaging of the data. K1 and K2 of the standard curve are calculated by solving simultaneous equations using mean AUC. K1 and K2 during expiration and inspiration are calculated, respectively. 718 subjects who had not been recently suffered from nasal diseases were examined by active anterior rhinomanometry. 47 functionally normal subjects in twenties were selected for calculation of the standard curve using the above mentioned method. In expiration, the values of K1 and K2 were 0.5476 and 1.3653, respectively. In inspiration, they were 0.4080 and 1.4750. Individual curve can be expressed by only one parameter. The normal range during nasal respiration is considered to be more than 0.7. The method presented in this study is convenient for the mutual comparison of the data both in clinical and basic research.
如今,呼吸过程中的鼻腔通畅度通常用鼻阻力来表示。然而,在整个呼吸阶段,鼻阻力并非恒定不变。因此,为便于数据的相互比较,确定表示阻力的参考点很有必要。鼻阻力测量标准化国际委员会一直在努力确定该参考点的设置位置,但尚未达成最终共识。本研究的目的是提出一种新方法来估计鼻腔呼吸传导率,而无需考虑参考点。鼻腔呼吸时的压力-流量曲线本质上非常相似,很少相互交叉。通过乘以标准方程V = n.f(P),不相交的抛物线曲线可以相互叠加。因此,n是比较这些曲线时唯一的参数。标准曲线确定如下。通过多项式回归分析检验了罗勒方程,并得出其足以模拟压力-流量曲线的结论。罗勒方程被转换为关于P的函数。沿P对该方程进行积分可得到曲线下面积(AUC)的值。总AUC可通过简单相加左右两侧的AUC获得。在横坐标上从原点到1.0和2.0进行定积分,可得到每条曲线中AUC的数值。通过对数据进行简单数学平均很容易计算出平均AUC。使用平均AUC通过解联立方程来计算标准曲线的K1和K2。分别计算呼气和吸气时的K1和K2。对718名近期未患鼻腔疾病的受试者进行了主动前鼻测压检查。选择47名20多岁功能正常的受试者,使用上述方法计算标准曲线。呼气时,K1和K2的值分别为0.5476和1.3653。吸气时,它们分别为0.4080和1.4750。个体曲线仅用一个参数即可表示。鼻腔呼吸时的正常范围被认为大于0.7。本研究提出的方法便于临床和基础研究中数据的相互比较。