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The appropriate geometrical arrangement of obstacles (noise barriers, walls, buildings etc.) can effectively reduce the influence of a sound source on a place of immission. Similar to the shadow of light, an acoustic shadow is formed behind the obstacle but is reduced by sound diffraction at the edges. Figure 2/15 gives a diagram of the shielding effect of a sound source. What determines the noise level reduction is the path length difference z. The path length difference is the diversion of the acoustic beam around an obstacle (z = A + B - b - a). The parameter z is substantially determined by the obstacle's effective height heff, but also by the distance of the barrier to the sound source. The path length difference is calculated according to the following formula: The noise level reduction through a barrier can be roughly estimated in accordance with the following equation: ∆Lz = 10 lg(3 + 0.12 · f · z) The frequency f in Hz is assumed at 500 Hz for industrial noises for example.
The diagram in figure 2/16 also allows for an estimation if heff and the distance e between sound source and place of immission (flat) are known. Thereby, hmax means the height of a place of immission above the street which can still be efficiently protected (depending on the width of the street and the distance of the place of immission to the street). More detailed calculation directives are given in VDI 2720-1, RLS-90 and Schall 03. Figure 2/16 shows that the wall does not completely hold off the sound but bends it at the top edge. As this is also true for the sides of the wall, a sufficient length is important here. This schematic representation also applies to noise protection barriers with the wall's top edge being replaced by the top of the barrier here. On the basis of the above-mentioned principles, the following indications and recommendations for the construction and structuring of barriers can be set up:
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