Suehiro M
Department of Otolaryngology, Okayama University Medical School.
Nihon Jibiinkoka Gakkai Kaiho. 1990 Mar;93(3):398-406. doi: 10.3950/jibiinkoka.93.398.
The effects of positive and negative pressure in the middle ear on tympanic membrane (TM) vibrations were studied in twenty canine temporal bones by holographic interferometry. The displacement of the TM was measured by moiré topography. 1) When pressure was applied to the tympanic cavity, the curvature of the TM became small under negative pressure and large under positive pressure, with the displacement being greater under positive pressure. 2) Without pressure load, the vibration pattern below 2 kHz was simple and there were peak displacement regions in the posterior and anterior parts of the membrane and the peaks occurred approximately halfway along the manubrium. The TM vibrations showed sectional patterns, above 3 kHz in the posterior and above 4 kHz in the anterior. The amplitude of the anterior peak was larger than that of the mallear tip, but smaller than that of the posterior. 3) At frequencies below 2 kHz, the vibration pattern was not affected by negative pressure load. At frequencies of 3 kHz or higher, the sectional patterns changed into the simpler patterns and the sectional vibrations diminished as the pressure increased. 4) Below 2 kHz, the TM amplitude decreased with increasing negative pressure. Above 3 kH, the amplitude showed an initial increase but decreased at higher negative pressure loading. With the amplitude of the mallear tip, the same tendency was observed. The resonance frequency shifted to a higher frequency range with pressure loading. 5) Under positive pressure, the vibration pattern remained unchanged below 2 kHz, and above 3 kH, sectional vibrations changed to the simple vibrations.(ABSTRACT TRUNCATED AT 250 WORDS)
通过全息干涉测量法,在20个犬颞骨上研究了中耳正压和负压对鼓膜(TM)振动的影响。用云纹地形测量法测量TM的位移。1)当向鼓腔施加压力时,TM的曲率在负压下变小,在正压下变大,正压下的位移更大。2)在无压力负荷时,2kHz以下的振动模式简单,膜的后部和前部有峰值位移区域,峰值大约出现在柄部的中间位置。TM振动呈现出分段模式,后部在3kHz以上,前部在4kHz以上。前部峰值的幅度大于锤骨尖端的幅度,但小于后部的幅度。3)在2kHz以下的频率,振动模式不受负压负荷的影响。在3kHz或更高频率时,分段模式变为更简单的模式,并且随着压力增加,分段振动减弱。4)在2kHz以下,TM幅度随着负压增加而减小。在3kHz以上,幅度最初增加,但在更高的负压负荷下减小。锤骨尖端的幅度也观察到相同的趋势。共振频率随着压力负荷转移到更高的频率范围。5)在正压下,2kHz以下的振动模式保持不变,在3kHz以上,分段振动变为简单振动。(摘要截断于250字)