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Book - School of Science and Technology

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Noise dispersal 467Table 16.8 Noise attenuation <strong>of</strong> plain ductworkDuct itemAttenuation(250 Hz)Straight ducts(dB/m run)150 150 mm 0.05600 600 mm 0.31800 1800 mm 0.2600 mm diameter 0.11800 mm diameter 0.03Square bends(dB/bend)150 mm depth 0300 mm 1450 mm 3600 mm 6BranchesAcoustic energy is dividedin ratio <strong>of</strong> duct areasThe attenuation in ducts depends on length <strong>and</strong> size: the longer the duct the greater theattenuation; the larger the duct the less the attenuation. The amount <strong>of</strong> attenuation maybe calculated from the data given in Table 16.8 <strong>and</strong> the accompanying notes, but for fullertreatment the Guide Section B12 should be consulted.Attenuation <strong>of</strong> sound energy at bends is a process <strong>of</strong> reflection back towards the source,rather than the absorption mechanism <strong>of</strong> straight duct runs. Radius bends, or mitre bendswith turning vanes generally give much less reduction than simple square bends.Where it is clear that residual sound will be too great, ducts may be lined withabsorption material either throughout or for certain lengths, as Figure 16.27. Suchmaterial must, <strong>of</strong> course, satisfy the requirements for fire protection <strong>and</strong> not erode whensubject to air flow.An approximate prediction for attenuation by use <strong>of</strong> an absorption lining to ducts isgiven by the formula:dB/m run ˆ D 1=4A15Absorbent liningAttenuation,dB/m105010 100 1000 10KFrequency, HzFigure 16.27 Acoustic insulation to ductwork

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