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Introduction to Acoustics

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130 Part A Propagation of Sound<br />

Part A 4.7<br />

tenuation with frequency and linear fits <strong>to</strong> the foliage<br />

attenuation.<br />

Often the insertion loss of tree belts alongside highways<br />

is considered relative <strong>to</strong> that over open grassland.<br />

An unfortunate consequence of the lower-frequency<br />

ground effect observed in mature tree stands is that the<br />

low-frequency destructive interference resulting from<br />

the relatively soft ground between the trees is associated<br />

with a constructive interference maximum at<br />

important frequencies (near 1 kHz) for traffic noise. Consequently<br />

many narrow tree belts alongside roads do<br />

not offer much additional attenuation of traffic noise<br />

compared with the same distances over open grassland.<br />

A Danish study found relative attenuation of 3 dB in<br />

the A-weighted Leq due <strong>to</strong> traffic noise for tree belts<br />

15–41 m wide [4.86]. Data obtained in the UK [4.87]<br />

indicates a maximum reduction of the A-weighted L10<br />

level due <strong>to</strong> traffic noise of 6 dB through 30 m of dense<br />

spruce compared with the same depth of grassland. This<br />

study also found that the effectiveness of the vegetation<br />

was greatest closest <strong>to</strong> the road. A relative reduction of<br />

5 dB in the A-weighted L10 level was found after 10 m of<br />

vegetation. For a narrow tree belt <strong>to</strong> be effective against<br />

traffic noise it is important that (a) the ground effect<br />

is similar <strong>to</strong> that for grassland, (b) there is substantial<br />

reduction of coherence between ground-reflected and direct<br />

sound at frequencies of 1 kHz and above, and that<br />

the attenuation through scattering is significant.<br />

If the belt is sufficiently wide then the resulting<br />

greater extent of the ground-effect dip can compensate<br />

for its low frequency. Through 100 m of red pine forest,<br />

Heisler et al. [4.88] have found 8 dB reduction in the<br />

A-weighted Leq due <strong>to</strong> road traffic compared with open<br />

grassland. The edge of the forest was 10 m from the edge<br />

of the highway and the trees occupied a gradual downward<br />

slope from the roadway extending about 325 m in<br />

each direction along the highway from the study site.<br />

Compared with open grassland Huisman [4.89] has predicted<br />

an extra 10 dB(A) attenuation of road traffic noise<br />

through 100 m of pine forest. He has remarked also that,<br />

whereas downward-refracting conditions lead <strong>to</strong> higher<br />

sound levels over grassland, the levels in woodland are<br />

comparatively unaffected. This suggests that extra attenuation<br />

obtained through the use of trees should be<br />

relatively robust <strong>to</strong> changing meteorology.<br />

Defrance et al. [4.90] have compared results from<br />

both numerical calculations and outdoor measurements<br />

for different meteorological situations. A numerical<br />

parabolic equation code has been developed [4.91] and<br />

adapted <strong>to</strong> road traffic noise situations [4.92] where<br />

road line sources are modeled as series of equivalent<br />

point sources of height 0.5 m. The data showed a reductioninA-weightedLeq<br />

due <strong>to</strong> the trees of 3 dB during<br />

downward-refracting conditions, 2 dB during homogeneous<br />

conditions and 1 dB during upward-refracting<br />

conditions. The numerical predictions suggest that in<br />

downward-refracting conditions the extra attenuation<br />

due <strong>to</strong> the forest is 2–6 dB(A) with the receiver at least<br />

100 m away from the road. In upward-refracting conditions,<br />

the numerical model predicts that the forest may<br />

increase the received sound levels somewhat at large<br />

distances but this is of less importance since levels at<br />

larger distances tend <strong>to</strong> be relatively low anyway. In<br />

homogeneous conditions, it is predicted that sound propagation<br />

through the forest is affected only by scattering<br />

by trunks and foliage. Defrance et al. [4.90] have concluded<br />

that a forest strip of at least 100 m wide appears <strong>to</strong><br />

be a useful natural acoustical barrier. Nevertheless both<br />

the data and numerical simulations were compared <strong>to</strong><br />

sound levels without the trees present, i. e., over ground<br />

from which the trees had simply been removed. This<br />

means that the ground effect both with and without trees<br />

would have been similar. This is rarely likely <strong>to</strong> be the<br />

case.<br />

A similar numerical model has been developed recently<br />

[4.93] including allowance for ground effect,<br />

wind speed gradient through foliage and assuming<br />

effective wave numbers deduced from multiple scattering<br />

theory for the scattering effects of trunks,<br />

branches and foliage. Again, the model predicts that<br />

the large wind speed gradient in the foliage tends<br />

<strong>to</strong> refract sound <strong>to</strong>wards the ground and has an important<br />

effect particularly during upwind conditions.<br />

However, neither of the PE models [4.91, 93] include<br />

back-scatter or turbulence effects. The neglect of the<br />

back-scatter is inherent <strong>to</strong> the PE, which is a oneway<br />

prediction method. While this is not a serious<br />

problem for propagation over flat ground because the<br />

back-scatter is small, nor over an impermeable barrier<br />

because the back-scattered field, though strong,<br />

does not propagate through the barrier, back scatter<br />

is likely <strong>to</strong> be significant for a forest. Indeed acoustic<br />

reflections from the edges of forests are readily<br />

detectable.

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