Overview
Engineering reference data for Outdoor Sound Partial Barriers in acoustics.
Key Formulas
Speed of Sound
Speed of sound in an ideal gas.
Sound Level
Decibel level.
Wavelength
Wavelength = speed / frequency.
Variables
| Symbol | Description | Unit |
|---|---|---|
| Speed of sound | m/s | |
| Sound level | dB | |
| Wavelength | m | |
| Frequency | Hz |
Sound-Barrier Interaction
When a barrier is interposed between a sound source and a receiver, the sound energy is affected in three ways:
- Reflected — Sound bounces back from the barrier surface
- Transmitted — Sound passes through the barrier material
- Diffracted — Sound bends around the edges of the barrier
The attenuation achieved by the barrier primarily depends on the diffraction component, which is quantified using the Fresnel number.
Fresnel Number Behavior
The Fresnel number determines the effectiveness of barrier attenuation:
where:
- (path length difference in m or ft)
Important characteristics:
- High frequencies (short wavelengths): The Fresnel number increases, resulting in greater attenuation
- Low frequencies (long wavelengths): The Fresnel number decreases toward zero, resulting in less attenuation
Note: The attenuation is reduced for moving sources (such as vehicles) compared to stationary sources.
Worked Example: Highway Noise Barrier
| Parameter | Value |
|---|---|
| Distance from highway to barrier top () | 20 m |
| Distance from barrier top to receiver () | 30 m |
| Direct distance source to receiver () | 43 m |
Step 1: Calculate path length difference:
Step 2: Calculate Fresnel numbers and attenuation:
| Frequency | Wavelength | Fresnel Number | Attenuation |
|---|---|---|---|
| 500 Hz | 0.69 m | ~17.5 dB | |
| 2000 Hz | 0.17 m | ~20 dB |
Higher frequencies achieve greater attenuation due to the increased Fresnel number.