dc.contributor.author |
Prospathopoulos, JM |
en |
dc.contributor.author |
Voutsinas, SG |
en |
dc.date.accessioned |
2014-03-01T01:25:56Z |
|
dc.date.available |
2014-03-01T01:25:56Z |
|
dc.date.issued |
2007 |
en |
dc.identifier.issn |
1095-4244 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/17821 |
|
dc.subject |
noise |
en |
dc.subject |
propagation |
en |
dc.subject |
wind turbine |
en |
dc.subject |
wind park |
en |
dc.subject |
ray theory |
en |
dc.subject |
complex terrain |
en |
dc.subject.classification |
Energy & Fuels |
en |
dc.subject.classification |
Engineering, Mechanical |
en |
dc.subject.other |
OUTDOOR SOUND-PROPAGATION |
en |
dc.subject.other |
PROFILE |
en |
dc.subject.other |
BOUNDARY |
en |
dc.subject.other |
LAYER |
en |
dc.title |
Application of a ray theory model to the prediction of noise emissions from isolated wind turbines and wind parks |
en |
heal.type |
journalArticle |
en |
heal.identifier.primary |
10.1002/we.211 |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1002/we.211 |
en |
heal.language |
English |
en |
heal.publicationDate |
2007 |
en |
heal.abstract |
Various propagation models have been developed to estimate the level of noise near residential areas. Predictions and measurements have proven that proper modelling of the propagation medium is of particular importance. In the present work, calculations are performed using a ray theory methodology. The ray trajectory, and transport equations are derived from the linear acoustics equations for a moving medium in three dimensions. Ground and atmospheric absorption, wave refraction and diffraction and atmospheric turbulence are taken into account by introducing appropriate coefficients in the equations. In the case of a wind turbine (WIT) it is assumed that noise is produced by a point source located at the rotor centre. Given the sound power spectrum, the noise spectrum at the receiver is obtained by solving the axisymmetric propagation problem. The procedure consists of (a) finding the eigenrays, (b) calculating the energy losses along the eigenrays and (c) synthesizing the sound pressure level (SPL) by superposing the contributions of the eigenrays. in the case of a wind park the total SPL is calculated by superposing the contributions of all W/Ts. Application is made to five cases of isolated W/Ts in terrains of varying complexity. In flat or even smooth terrain the predictions agree well with the measurements. In complex terrain the predictions can be considered satisfactory, taking into account the assumption of constant wind velocity profile. Application to a wind park shows clearly the influence of the terrain on the wind velocity and consequently on the SPL. Copyright (C) 2006 John Wiley & Sons, Ltd. |
en |
heal.publisher |
JOHN WILEY & SONS LTD |
en |
heal.journalName |
WIND ENERGY |
en |
dc.identifier.doi |
10.1002/we.211 |
en |
dc.identifier.isi |
ISI:000245481200001 |
en |
dc.identifier.volume |
10 |
en |
dc.identifier.issue |
2 |
en |
dc.identifier.spage |
103 |
en |
dc.identifier.epage |
119 |
en |