Environmental Engineering Reference
In-Depth Information
Figure 9: Diffraction behind obstacles high-frequency (left) and low-frequency
(right) waves.
rise to noise (Fig. 8f). One commonly divides the noise due to atmospheric
turbulence into a low-frequency regime (when the length-scale of the fl uctuations
is much larger than the size of the body) and a high frequency regime (the length-
scale of the fl uctuations is much smaller then the airfoil). As it will be shown in
Section 6.2, these two regimes can be treated separately in noise modeling [4].
Due to the chaotic behavior of turbulence, these models are not deterministic.
According to Lowson [9], the self-noise sources dominate at low wind speeds,
near cut-in, while at the rated power the turbulence inlet noise source dominates.
A detailed description of all these noise mechanisms can be found, e.g. in [4].
4.2 Propagation
In the previous section the noise generation mechanisms have been discussed. The
knowledge of these noise
sources
, however, is not enough to predict the sound
pressure level at a receiver. While the acoustic waves are traveling through the
atmosphere, several factors infl uence the propagated sound pressure levels, the
most important ones being the followings:
•
The
distance
to the receiver. For increasing distance the acoustic energy is
spread in a larger volume which decreases the sound pressure level.
•
Absorption
is due to the air viscosity and converts the acoustic energy into heat.
•
Refl ections
due to the ground and surrounding objects.
When a wave passes around a solid object
•
diffraction
occurs. For high frequen-
cies (wavelength much smaller than the object size) a shadow zone occurs
behind the object. The shadow zone decreases with decreasing frequency, com-
pletely disappearing for wavelengths much larger than the size of the object
(see Fig. 9).
•
Refractions
are caused due to temperature gradients which cause different
densities in different layers of the air, and as a consequence impose different
propagation speeds of the sound waves.
The
•
wind speed and direction
infl uences the directivity of the noise propagation.
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