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  Vol. 113 No. 3, March 1987 TABLE OF CONTENTS
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Acoustic Impedance Transformation-Reply

RICHARD L. GOODE, MD
Stanford, Calif

Arch Otolaryngol Head Neck Surg. 1987;113(3):329.

Since this article does not have an abstract, we have provided the first 150 words of the full text PDF and any section headings.

In Reply.—Dr Kimberley is incorrect when he states that "a mechanical/acoustical system such as the external ear is quite incapable of impedance transformation, at any frequency." One way to model the acoustic function of the external ear is as a small horn whose mouth contacts the low specific impedance air of the external environment (41.5 acoustic {Omega}, cm/g/s), while the throat ends at the higher impedance tympanic membrane (TM), typically around 450 acoustic {Omega}, cm/ g/s. The knowledge that horns act as impedance-matching devices in this situation was first described in 19191 and is well covered in acoustics texts.2,3

I prefer to think of the external ear functioning as a quarter wavelength pipe resonator closed at one end by the TM and connected to a cavity resonator at the other. The pressure gain at the TM in the resonant frequency range (2500 to 6000 Hz) almost completely offsets . . . [Full Text PDF of this Article]



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