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Specific Acoustic Impedance

Reference data and engineering information about specific acoustic impedance for acoustics applications.

specificacousticimpedance

Overview

Engineering reference data for Specific Acoustic Impedance in acoustics.

Key Formulas

Speed of Sound

c=γRTc = \sqrt{\gamma R T}

Speed of sound in an ideal gas.

Sound Level

L=10log10(I/I0)L = 10 \log_{10}(I/I_0)

Decibel level.

Wavelength

λ=c/f\lambda = c / f

Wavelength = speed / frequency.

Variables

SymbolDescriptionUnit
ccSpeed of soundm/s
LLSound leveldB
λ\lambdaWavelengthm
ffFrequencyHz

Physical Significance

Specific acoustic impedance (Z) quantifies the inherent resistance a medium offers to the propagation of sound. The relationship Z = ρc underscores that this property is determined solely by the medium's density (ρ) and the speed of sound (c) within it, not by the sound wave's characteristics. It defines the coupling between the sound pressure (p) and the resulting particle velocity (v).

Key Relationships & Properties

The fundamental formula relates impedance, pressure, and velocity: Z=pv=ρcZ = \frac{p}{v} = \rho c

For a plane wave traveling through a medium, the specific acoustic impedance is a real number. In more complex scenarios involving viscous or reactive media, it can be a complex quantity: Z=R+iXZ = R + iX where R is the resistive (real) part and X is the reactive (imaginary) part.

The impedance is also related to the medium's bulk modulus (K) through the relationship: c=KρZ=ρKρ=ρKc = \sqrt{\frac{K}{\rho}} \quad \Rightarrow \quad Z = \rho \sqrt{\frac{K}{\rho}} = \sqrt{\rho K}

Impedance Mismatch and Acoustic Effects

A critical concept is the impedance mismatch at the boundary between two media with different specific acoustic impedances (Z₁ and Z₂). This mismatch governs the reflection and transmission of sound energy.

  • Reflection Coefficient (R): R=Z2Z1Z2+Z1R = \frac{Z_2 - Z_1}{Z_2 + Z_1}
  • Transmission Coefficient (T): T=2Z2Z2+Z1T = \frac{2 Z_2}{Z_2 + Z_1}

A large difference between Z₁ and Z₂ results in strong reflection, which is why air (Z ≈ 415 Pa·s/m) and water (Z ≈ 1.5 × 10⁶ Pa·s/m) are nearly perfect reflectors of sound at their interface.

Representative Values

The table below provides orders of magnitude for common materials at standard conditions.

5 rows
Representative specific acoustic impedance values for common media.
Medium
Density (ρ)(kg/m³)
Speed of Sound (c)(m/s)
Specific Acoustic Impedance (Z)(Pa·s/m)
Air (20°C)1.21343415
Water (20°C)99814811.48 × 10⁶
Seawater102515001.54 × 10⁶
Steel (longitudinal)780050003.9 × 10⁷
Human tissue (average)106015401.63 × 10⁶

Source: engineeringtoolbox.com

Interactive Charts

Air - Speed of Sound vs. Temperature

References