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Sound pressure distribution and power flow within the gerbil ear canal from 100 Hz to 80 kHz

机译:沙土鼠耳道内的声压分布和功率流从100 Hz到80 kHz

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摘要

Sound pressure was mapped in the bony ear canal of gerbils during closed-field sound stimulation at frequencies from 0.1 to 80 kHz. A 1.27-mm-diam probe-tube microphone or a 0.17-mm-diam fiber-optic miniature microphone was positioned along approximately longitudinal trajectories within the 2.3-mm-diam ear canal. Substantial spatial variations in sound pressure, sharp minima in magnitude, and half-cycle phase changes occurred at frequencies >30 kHz. The sound frequencies of these transitions increased with decreasing distance from the tympanic membrane (TM). Sound pressure measured orthogonally across the surface of the TM showed only small variations at frequencies below 60 kHz. Hence, the ear canal sound field can be described fairly well as a one-dimensional standing wave pattern. Ear-canal power reflectance estimated from longitudinal spatial variations was roughly constant at 0.2–0.5 at frequencies between 30 and 45 kHz. In contrast, reflectance increased at higher frequencies to at least 0.8 above 60 kHz. Sound pressure was also mapped in a microphone-terminated uniform tube—an “artificial ear.” Comparison with ear canal sound fields suggests that an artificial ear or “artificial cavity calibration” technique may underestimate the in situ sound pressure by 5–15 dB between 40 and 60 kHz.
机译:在从0.1到80 kHz的频率进行封闭场声刺激期间,在沙鼠的骨耳道中绘制了声压。将直径为1.27毫米的探头管麦克风或直径为0.17毫米的光纤微型麦克风沿着直径为2.3毫米的耳道内的大致纵向轨迹放置。大于30 kHz的频率会发生声压的巨大空间变化,极小的幅度和半周期相位变化。这些过渡的声音频率随着与鼓膜(TM)距离的减小而增加。在TM表面上正交测量的声压在低于60 kHz的频率下仅显示出很小的变化。因此,耳道声场可以很好地描述为一维驻波模式。根据纵向空间变化估计的耳道功率反射率在30至45 kHz的频率下大致恒定在0.2-0.5。相反,在更高的频率下,反射率在60 kHz以上至少增加到0.8。声压也被映射到麦克风端接的均匀管中,即“人造耳”。与耳道声场的比较表明,人工耳或“人工腔校准”技术可能会低估40至60 kHz之间的原位声压5–15 dB。

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