Abstract

In this work, we present an integrated photogrammetric-acoustic technique that, together with the construction of a scaled wind tunnel, allows us to experimentally analyze the permeability behavior of a new type of acoustic screen based on a material called sonic crystal. Acoustic screens are devices used to reduce noise, mostly due to communication infrastructures, in its transmission phase from the source to the receiver. The main constructive difference between these new screens and the classic ones is that the first ones are formed by arrays of acoustic scatterers while the second ones are formed by continuous walls. This implies that, due to their geometry, screens based on sonic crystals are permeable to wind and water, unlike the classic ones. This fact may allow the use of these new screens in sandy soils, where sand would pass through the screen, avoiding the formation of sand dunes that are formed in classic screens and drastically reducing their acoustic performance. In this work, the movement of the sand and the resulting acoustic attenuation in these new screens are analyzed qualitatively, comparing the results with those obtained with the classic ones, and obtaining interesting results from the acoustic point of view.

Highlights

  • Noise can be defined as an unwanted or unpleasant outdoor sound generated by human activity, and is one of the main environmental problems all over the world [1]

  • The experimental protocol was developed as follows: First, the sand reservoir of the scaled wind tunnel was filled with 10 cm of clean and sieved sand

  • To quantitatively estimate the amount of sand moved in this comparison, we considered three longitudinal sections of the scaled wind tunnel, as can be seen on the left side of Figure 7a

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Summary

Introduction

Noise can be defined as an unwanted or unpleasant outdoor sound generated by human activity, and is one of the main environmental problems all over the world [1]. This kind of pollution can be controlled in each of the three phases into which its propagation is divided: (i) Noise generation at the source; (ii) transmission of noise from the source to the receiver, and (iii) noise reception.

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