Gavriely N, Palti Y, Alroy G, Grotberg J B
J Appl Physiol Respir Environ Exerc Physiol. 1984 Aug;57(2):481-92. doi: 10.1152/jappl.1984.57.2.481.
We measured the time and frequency domain characteristics of breath sounds in seven asthmatic and three nonasthmatic wheezing patients. The power spectra of the wheezes were evaluated for frequency, amplitude, and timing of peaks of power and for the presence of an exponential decay of power with increasing frequency. Such decay is typical of normal vesicular breath sounds. Two patients who had the most severe asthma had no exponential decay pattern in their spectra. Other asthmatic patients had exponential patterns in some of their analyzed sound segments, with a range of slopes of the log power vs. log frequency curves from 5.7 to 17.3 dB/oct (normal range, 9.8-15.7 dB/oct). The nonasthmatic wheezing patients had normal exponential patterns in most of their analyzed sound segments. All patients had sharp peaks of power in many of the spectra of their expiratory and inspiratory lung sounds. The frequency range of the spectral peaks was 80-1,600 Hz, with some presenting constant frequency peaks throughout numerous inspiratory or expiratory sound segments recorded from one or more pickup locations. We compared the spectral shape, mode of appearance, and frequency range of wheezes with specific predictions of five theories of wheeze production: 1) turbulence-induced wall resonator, 2) turbulence-induced Helmholtz resonator, 3) acoustically stimulated vortex sound (whistle), 4) vortex-induced wall resonator, and 5) fluid dynamic flutter. We conclude that the predictions by 4 and 5 match the experimental observations better than the previously suggested mechanisms. Alterations in the exponential pattern are discussed in view of the mechanisms proposed as underlying the generation and transmission of normal lung sounds. The observed changes may reflect modified sound production in the airways or alterations in their attenuation when transmitted to the chest wall through the hyperinflated lung.
我们测量了7名哮喘患者和3名非哮喘性喘息患者呼吸音的时域和频域特征。评估了喘息声的功率谱,包括频率、幅度、功率峰值的时间以及功率随频率增加的指数衰减情况。这种衰减是正常肺泡呼吸音的典型特征。两名哮喘最严重的患者其频谱中没有指数衰减模式。其他哮喘患者在一些分析的声音段中呈现指数模式,对数功率与对数频率曲线的斜率范围为5.7至17.3 dB/倍频程(正常范围为9.8 - 15.7 dB/倍频程)。非哮喘性喘息患者在大多数分析的声音段中具有正常的指数模式。所有患者在其呼气和吸气肺音的许多频谱中都有尖锐的功率峰值。频谱峰值的频率范围为80 - 1600 Hz,一些在从一个或多个采集位置记录的多个吸气或呼气声音段中呈现恒定频率峰值。我们将喘息声的频谱形状、出现方式和频率范围与五种喘息产生理论的具体预测进行了比较:1)湍流诱导壁式谐振器,2)湍流诱导亥姆霍兹谐振器,3)声刺激涡旋声(哨声),4)涡旋诱导壁式谐振器,5)流体动力颤振。我们得出结论,理论4和理论5的预测比先前提出的机制更符合实验观察结果。鉴于作为正常肺音产生和传播基础所提出的机制,讨论了指数模式的改变。观察到的变化可能反映了气道中声音产生的改变或声音通过过度充气的肺传输到胸壁时其衰减的改变。