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Introduction to Acoustics

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Table 23.8 Crossover speeds for various cases. According<br />

<strong>to</strong> Sandberg [23.99] “The table assumes that ‘normal’ tires<br />

are used, and that the road surface is a dense asphalt concrete<br />

or an SMA with max 10-14 mm chippings. ‘Cruising’ is<br />

constant speed, and ‘Accelerating’ means an ‘average’ way<br />

of accelerating after a s<strong>to</strong>p, but not as much as in the ISO<br />

362 driving mode.” (After [23.99] Table 5.1)<br />

Vehicle type Cruising Accelerating<br />

Cars made 1985-95 30–35 km/h 45–50km/h<br />

Cars made 1996- 15–25 km/h 30–45km/h<br />

Heavy trucks made 40–50 km/h 50–55km/h<br />

1985-1995<br />

Heavy trucks made 1996- 30–35 km/h 45–50km/h<br />

of the tire treads, axial vibrations of the sidewalls, air<br />

pumping due <strong>to</strong> the deformation of the tread by irregularities<br />

in the road surface, and possibly vibration of the<br />

rim of the tire. At low frequencies, there is evidence that<br />

the tire treadband can be considered <strong>to</strong> be a cylindrical<br />

beam elastically supported by the sidewall [23.100].<br />

A quantative description of tire–road noise is best<br />

obtained by development of a model of the sound radiation.<br />

A his<strong>to</strong>ry of past modeling attempts has been<br />

given by Kuijpers and van Blokland [23.101], and more<br />

generalized models are also available [23.102, 103].<br />

The road surface itself has a significant effect on the<br />

generation of tire noise. The roughness of the surface<br />

affects the excitation of the tire and subsequent generation<br />

of noise; the porosity of the surface effectively<br />

changes the compressibility of trapped air, and if the<br />

acoustic impedance is in the range <strong>to</strong> absorb sound, energy<br />

can be absorbed by the surface. Information on the<br />

characteristics of porous surfaces is given in [23.99].<br />

Tire–road interaction noise is currently the subject<br />

of intensive research. Bernhard et al. have given a summary<br />

of research [23.104], Sandberg et al. [23.105]<br />

have discussed poroelastic road surfaces, and Thorn<strong>to</strong>n<br />

et al. [23.106] have studied the variability of existing<br />

pavements. Although porous surfaces have been shown<br />

<strong>to</strong> provide noticeable reductions in traffic noise levels,<br />

questions remain about the durability of these surfaces,<br />

especially in cold climates. The durability of such surfaces<br />

in a warm climate has been studied by Donavan<br />

et al. [23.107].<br />

Traffic Noise Prediction Models. The US Federal Highway<br />

Administration has released version 2.5ofthetraffic<br />

noise model, whichmaybeusedforawidevarietyof<br />

calculations related <strong>to</strong> traffic noise. The characteristics<br />

Noise 23.2 Noise Sources 989<br />

of the model are described in Sect. 23.3.1 on outdoor<br />

noise barriers.<br />

Aircraft Noise<br />

Exterior noise emissions of aircraft are of major importance<br />

<strong>to</strong> persons on the ground, and interior noise emissions<br />

are a concern of both airline passengers and crews.<br />

Aircraft Noise Emissions. Noise emissions from civil<br />

aircraft have been regulated for more than 35 years, first<br />

by the Federal Aviation Administration in the United<br />

States, and later, internationally, by the International<br />

Civil Aviation Organization (ICAO). Nevertheless, although<br />

the noise from individual airplanes has been<br />

significantly reduced, the <strong>to</strong>tal exposure <strong>to</strong> aircraft noise<br />

for residents in communities near many airports has<br />

increased because of the growth in the number of<br />

aircraft operations at airports throughout the world. Consequently,<br />

opera<strong>to</strong>rs of the airplanes and the airports<br />

continue <strong>to</strong> face limitations because of aircraft noise.<br />

This section discusses the noise emissions of aircraft;<br />

noise at the receiver is discussed in Sect. 23.4.4. Requirements<br />

for the noise levels that may be produced by<br />

aircraft are given in title 14 of the US Code of Federal<br />

Regulations, 14CFR part 36 [23.108] and in annex 16 <strong>to</strong><br />

the Convention on International Civil Aviation (ICAO<br />

annex 16) [23.109].<br />

The methodology of determining the noise emission<br />

of aircraft for certification purposes is well developed.<br />

Certification noise levels are not intended <strong>to</strong>, and do<br />

not, represent noise levels that may be measured in<br />

communities around airports.<br />

Certification noise limits, in terms of effective perceived<br />

noise level (EPNL), are specified at three points<br />

– known as lateral, flyover, and landing approach.<br />

The limits are a function of the maximum design<br />

takeoff gross mass, and apply <strong>to</strong> both jet-powered<br />

and propeller-driven transport-category airplanes, business/executive<br />

airplanes, and helicopters. The limits<br />

apply <strong>to</strong> new-design airplanes and <strong>to</strong> retrofit modifications<br />

of old-design aircraft.<br />

Perceived noise levels are determined from 500 msaverage<br />

one-third-octave-band sound pressure levels, at<br />

500 ms intervals, and are adjusted for the additional<br />

noisiness caused by prominent <strong>to</strong>nes, if present, or<br />

other spectral irregularities. For each of the three noisemeasurement<br />

points, effective perceived noise levels are<br />

determined from the time integral of <strong>to</strong>ne-corrected perceived<br />

noisiness and adjusted <strong>to</strong> reference atmospheric<br />

conditions, reference flight paths, reference airspeeds,<br />

and reference engine power settings.<br />

Part G 23.2

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