Bilingual edition: English is preserved and Chinese follows each unit. Terminology uses the confirmed v20260916 glossary; automated semantic review remains traceable.
中英双语版:英文原文完整保留,中文紧随对应单元;术语采用 v20260916 确认表,自动语义审校结果可追溯。

Acoustic Impedance

声阻抗

The concept of acoustic impedance is useful for a materials for calculating reflection and transmission coefficients for sound or pressure waves at material interfaces. It can be defined macroscopically for a given medium geometry as Z=p/U where p=acoustic pressure and U = acoustic volume flow, or defined as an intensive property of a medium, where z = specific acoustic impedance:

声阻抗的概念对于计算声或压力波在材料界面处的反射系数和透射系数非常有用。它可以定义为给定介质几何的宏观量,即 Z = p/U,其中 p 为声压,U 为声体积流量,或者定义为介质的强度性质,其中 z = 特定声阻抗:

This treatment will be limited to the specific acoustic impedance. See the references below for a more general treatment. For a sound wave, the particle displacement y as a function of time is of the form

本处理将限于特定的声阻抗。请参见下面的参考文献以获得更一般的处理。对于声波,粒子位移y作为时间函数的形式为

and the associated velocity v and pressure p may be written

以及相关的速度 v 和压力 p 可以表示为

where B is the adiabatic bulk modulus of the material. Substituting into the defining relationship for z gives

其中 B 是材料的绝热体积模量。将其代入 z 的定义关系得

which reduces to

这可简化为

This is a convenient form for calculating reflection and transmission coefficients for sound waves.

这是计算声波反射系数和透射系数的一种方便形式。

References:

参考文献:

Acoustic impedance, intensity and power

声阻抗、声强和功率

The wave equation for sound

声波的波动方程
Index

索引
 
HyperPhysics***** Sound
HyperPhysics ***** 声音
R Nave
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