Laserfiche WebLink
Enbridge Energy, LP Hoover& Keith, Inc. <br /> Waterloo Pump Station—Noise Impact Analysis RN 3083/JN 4796 <br /> APPENDIX B— Estimated Contribution of Station (10/10/14) <br /> ANALYSIS METHODOLOGY AND SOURCE OF SOUND DATA <br /> In general, the predicted sound level contributed by the pumping station equipment was calculated as a <br /> function of frequency from estimated unweighted octave-band ("O.B.") sound power levels ("PWLs")for <br /> each significant sound source. The following summarizes the acoustical analysis procedure for the <br /> Station: <br /> ➢ Initially, unweighted O.B. PWL values of the significant noise sources were determined from <br /> equipment manufacturer's sound data and/or actual sound level measurements performed by H&K at <br /> similar type of equipment/components expected for this facility. <br /> ➢ Then, expected noise reduction (NR) or attenuation in dB per O.B. frequency due to any noise control <br /> measures, hemispherical sound propagation (discussed in more detail below*) and atmospheric sound <br /> absorption (discussed in more detail below**)were subtracted from the unweighted O.B. PWLs to <br /> obtain the unweighted O.B. SPLs of each noise source. The sound attenuation effect due to shielding <br /> by buildings and/or enclosures has been conservatively ignored. The sound attenuation effect due to <br /> foliage or land contour was not considered in the analysis since there is probably minimum attenuation <br /> due to foliage. <br /> ➢ Finally, the resulting estimated unweighted O.B. SPLs for all noise sources associated with the Station <br /> (with noise control and other sound attenuation effects)were logarithmically summed, and the total <br /> O.B. SPLs for all noise sources were corrected for A-weighting to provide the estimated overall A-wt. <br /> sound level contributed by the Station at the Property Line. <br /> *Attenuation due to hemispherical sound propagation: Sound propagates outwards in all directions (i.e., <br /> length, width, height)from a point source, and the sound energy of a noise source decreases with <br /> increasing distance from the source. In the case of hemispherical sound propagation, the source is <br /> located on a flat continuous plane/surface(e.g., ground), and the sound radiates hemispherically(i.e., <br /> outward, over and above the surface)from the sound source. The following equation is the theoretical <br /> decrease of sound energy when determining the resulting SPL values of a noise source at a specific <br /> distance("r") of a receiver from the estimated PWL values: <br /> Decrease in SPL("hemispherical propagation")from a noise source= 20*log(r)—2.3 dB <br /> where"r" is distance of the receiver from the noise source. <br /> **Attenuation due to air absorption:Air absorbs sound energy, and the amount of absorption <br /> ("attenuation") is dependent on the temperature and relative humidity(R.H.)of air and frequency of sound. <br /> For example, the attenuation due to air absorption for 1000 Hz O.B. SPL is approximately 1.5 dB per <br /> 1,000 feet for standard day conditions(i.e., no wind, 60 deg. F. and 70%or 50% R.H.). <br /> The estimated unweighted O.B. PWLs of the motor-driven pumps, piping, substation equipment and any <br /> other site equipment were estimated from field sound measurements by H&K on similar equipment and/or <br /> from sound data provided by the equipment manufacturer. <br /> B-3 <br />