Sound Attenuation - Interactive Visualization

Interactive simulation demonstrating how sound intensity decreases with distance and medium absorption

1m
2m
3m
4m
🔊
Source
Intensity: High → Low
Wavefront

Decibel Meter

90.0 dB
0 30 60 90 120

Intensity Information

Source Intensity (I₀): 1.00 W/m²
Current Distance: 1.0 m
Current Intensity: 1.00 W/m²
Attenuation: 0.0 dB

Parameters

Active Formula

I = I₀ / r²
Inverse square law: Intensity decreases with the square of distance

Intensity at Different Distances

Distance (m) Intensity (W/m²) Level (dB)

Mathematical Foundation

Geometric Spreading (Free Field)

I = I₀ / r²

Sound energy spreads over a sphere with surface area 4πr². Intensity decreases inversely with the square of distance from the source.

Medium Absorption

I = I₀ · e^(-αx)

Sound energy is absorbed by the medium as it travels. The absorption coefficient α determines how quickly intensity decreases exponentially with distance.

Combined Effect

I = I₀ · e^(-αx) / r²

In real environments, both geometric spreading and medium absorption contribute to sound attenuation.

Sound Pressure Level

SPL = 20·log₁₀(P/P₀) = 10·log₁₀(I/I₀)

Decibels provide a logarithmic scale that better matches human hearing perception. A 10 dB increase represents a 10× intensity increase.

What is Sound Attenuation?

Sound attenuation is the reduction in sound intensity as it travels through a medium. This occurs due to two primary mechanisms: geometric spreading, where sound energy distributes over a larger area as it propagates, and medium absorption, where the medium itself converts sound energy into heat. Understanding sound attenuation is crucial for acoustic design, noise control, and audio engineering.

Inverse Square Law

In a free field (no reflections), sound intensity follows the inverse square law: I = I₀/r². This means doubling the distance reduces intensity to one-quarter (a 6 dB drop). This geometric spreading occurs because sound energy spreads over the surface of an expanding sphere with area 4πr².

Absorption in Media

Different media absorb sound at different rates. Air absorbs high frequencies more than low frequencies, with absorption increasing with humidity. Water is much denser and absorbs sound more quickly than air, which is why sonar has limited range. The absorption coefficient α determines the rate of exponential decay.

Real-World Applications

  • Concert Hall Design: Architects use attenuation principles to ensure even sound distribution throughout a venue, balancing reflections and absorption.
  • Noise Barriers: Highway noise walls and soundproofing materials are designed based on attenuation calculations to reduce environmental noise pollution.
  • Audio Engineering: Sound engineers account for attenuation when placing microphones and designing speaker systems to achieve optimal sound quality.
  • Underwater Acoustics: Sonar systems and submarine communication must account for high attenuation in water, limiting effective range.
  • Building Acoustics: Understanding attenuation helps design spaces with appropriate reverberation times and sound isolation between rooms.

Human Hearing Perception

Threshold of Hearing

0 dB is the threshold of human hearing at 1 kHz. Normal conversation is about 60 dB, while pain begins around 120-140 dB.

Logarithmic Perception

Humans perceive loudness logarithmically. A 10 dB increase sounds roughly twice as loud, even though intensity increases 10×.

Frequency Dependence

Human hearing is most sensitive around 3-4 kHz and less sensitive at very low and very high frequencies.