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The Problem of Noise Reduction with Reference ... - CAFE Foundation

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This term gives the distance effect. From figure 3 thevalue <strong>of</strong> the last term is 10 loglo ‘qn2 = -16 forv&a two-blade propeller at - = o.oll~~e <strong>The</strong> appropriateMach number is obtained bycusing the 0.8 radius as areference -. station and disregarding the forward speed.Thus, : = o.8~ = 0.455,.<strong>The</strong> sound inteniity due to the propeller can”nowbe obtained sirmly by adding the four terms on the righthand side <strong>of</strong> equation (10). J.nthe order given, therirst <strong>of</strong> these terms is a constant, the second is due tothe disk loading and. Mach number <strong>of</strong> the al.i’qlaneandthe propeller, the third takss into account the distancefrom the propeller, and the fourth is a function obtainedfrom f’lgure3 for various values <strong>of</strong> v/c and variousnumbers <strong>of</strong> blades. In the foregoing example, tbrefore,the sound intensity at a distance cf 1 radius from the .propeller isI =118.6+12-0-16 = 114..6“ daclbelsAt a distance <strong>of</strong> 300 feet the sound intensity <strong>of</strong>propeller isthe samei—- .—.I = 118.6 + 12 -Lo - 16 = 74..6 decibels‘I%epropeller sound intensities have also been calculatedfor a somewhat larger airplane, which will becalld airplane B, having the following specifications:Airplane speed, miles per hour . . . . . . . . . . 165HorseDower. . , . . . . . . . . . . . . . . . . . Ij3Propeller speed~ rpm . . . . . . . . . . . . . . . ~~r)()Propeller dianeter, feet . . , . i . , . . . . . . 5.5‘Ihedetailed calculations for airplane B are omitted.For comparison. the calculated ~roneller soundintensities ;or aifilsnes A and 1 at’a distance <strong>of</strong> 3 feetand 300 feet, respectively, are ~ .ven asAirplaneABI at3f~t114.6127I at~OC) feet(db)k*7i7.,..10❑■

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