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Outdoor propagation – cylindrical field

Outdoor propagation – cylindrical field. Line Sources. Many noise sources found outdoors can be considered line sources: roads, railways, airtracks, etc. Geometry for propagation from a line source to a receiver in this case the total power is dispersed over a cylindrical surface:.

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Outdoor propagation – cylindrical field

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  1. Outdoor propagation – cylindrical field

  2. Line Sources Many noise sources found outdoors can be considered line sources: roads, railways, airtracks, etc. • Geometry for propagation from a line source to a receiver • in this case the total power is dispersed over a cylindrical surface: In which Lw’ is the sound power level per meter of line source

  3. Coherent cylindrical field • The power is dispersed over an infinitely long, pulsating cylinder: L r In which Lw’is the sound power level per meter of line source

  4. “discrete” (and incoherent) linear sources Another common case is when a number of point sources are located along a line, each emitting sound mutually incoherent with the others: • Geometry of propagation for a discrete line source and a receiver • We could compute the SPL at the receiver as the energetic (incoherent) summation of many spherical wavefronts. But at the end the result shows that SPL decays with the same cylindrical law as with a coherent source: Lw’ The SPL reduces by 3 dB for each doubling of distance d. Note that the incoherent SPL is 2 dB louder than the coherent one!

  5. Example of a discrete line source: cars on the road Distance a between two vehicles is proportional to their speed: In which V isspeed in km/h and Nis the number of vehiclespassing in 1 h • The sound powerlevelLWp of a single vehicleis: • Constant up to 50 km/h • Increases linearly between 50 km/h and 100 km/h (3dB/doubling) • Above 100 km/h increases with the square of V (6dB/doubling)

  6. Example of a discrete line source: cars on the road • Hence there is an “optimal” speed, which causes the minimum value of SPL, which lies around 70 km/h • Modern vehicles have this “optimal speed” at even larger speeds, for example it is 85 km/h for the Toyota Prius

  7. Outdoors propagation – excess attenuation

  8. Free field: excess attenuation • Other factors causing additional attenuation during outdoors progation are: • air absorption • absorption due to presence of vegetation, foliage, etc. • metereological conditions (temperature gradients, wind speed gradients, rain, snow, fog, etc.) • obstacles (hills, buildings, noise barriers, etc.) • All these effects are combined into an additional term L, in dB, which is appended to the free field formula: •  LI = Lp = LW - 20 log r - 11 + 10 log Q - L (dB) • Most of these effects are relevant only at large distance form the source. The exception is shielding (screen effect), which instead is maximum when the receiver is very close to the screen

  9. Excess attenuation: temperature gradient Shadow zone

  10. Excess attenuation: wind speed gradient

  11. Excess attenuation: air absorption Air absorption coefficients in dB/km (from ISO 9613-1 standard) for different combinations of frequency, temperature and humidity:

  12. Excess attenuation – barriers

  13. Noise screens (1) • A noise screen causes an insertion lossL: • L = (L0) - (Lb) (dB) • where Lb and L0 are the values of the SPL with and without the screen. • In the most general case, there arey many paths for the sound to reach the receiver when the barrier is installed: • diffraction at upper (B) and side (C,D)edges of the screen • passing through the screen (SA), • reflection over other surfaces present in proximity (building, etc. - SEA). 

  14. Noise screens (2): the MAEKAWA formulas • If we only consider the enrgy diffracted by the upper edge of an infinitely long barrier we can estimate the insertion loss as: • L= 10 log (3+20 N) for N>0 (point source) • L = 10 log (2+5.5 N) for N>0 (linear source) • where N is Fresnel number defined by:  • in which  is the wavelength and  is the path difference among the diffracted and the direct sound.

  15. Maekawa chart

  16. Noise screens (3): finite length • If the barrier is not infinite, we need also to consider its lateral edges, each with its Fresnel number (N1, N2), and we have: • L = Ld - 10 log (1 + N/N1 + N/N2) (dB) • Valid for values of N, N1, N2 > 1. • The lateral diffraction is only sensible when the side edge is closer to the source-receiver path than 5 times the “effective height”. heff R S

  17. Noise screens (4) • Analysis: • The insertion loss value depends strongly on frequency: • low frequency  small sound attenuation. • The spectrum of the sound source must be known for assessing the insertion loss value at each frequency, and then recombining the values at all the frequencies for recomputing the A-weighted SPL. SPL (dB) No barrier – L0 = 78 dB(A) Barrier – Lb = 57 dB(A) f (Hz)

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