Determination of The Scattering Parameters of Fittings in Industrial Buildings for Use in Computer Based Factory Noise Prediction Models: Part 2 – Scale Model Experiments

1995 ◽  
Vol 2 (3) ◽  
pp. 527-548 ◽  
Author(s):  
H.A. Akil ◽  
D.J Oldham

In a companion paper results obtained from computer simulation1 have demonstrated that the sound propagation characteristics of disproportionate rooms are determined by the product of the fitting parameters scattering cross-section (Q) and absorption coefficient (αobst) of fittings. It was also proposed that the absorption of a fitting as measured in a conventional reverberation chamber is equivalent to four times the product of those two parameters. This suggests that measurement of fitting absorption in a conventional reverberation chamber could provide the data required for input into current computer based factory noise prediction models. Since both parameters are required as inputs to computer models it would be necessary to separate them in some way from the data obtained in the reverberation chamber. In this paper two methods for determining the scattering parameters of fittings in industrial buildings based upon acoustical measurements are described. The accuracy of these is compared with that resulting from the application of a geometrical measurement method to determine the scattering cross-section (Q) of various shapes of model scatterers employed in experimental work employing 1:20 acoustic scale models. The values of Q obtained from each method were used to predict sound characteristics a model disproportionate chamber using RAYSCAT. The predicted results obtained from the computer model by inputting the values of Q determined using the acoustical measurement methods were found to be more accurate than those using the geometrical measurement method.

1995 ◽  
Vol 2 (2) ◽  
pp. 461-481 ◽  
Author(s):  
H.A. Aldi ◽  
D.J. Oldham

In this the first of two companion papers, it is established that the accepted view amongst researchers is that models in which the scatterers of sound in industrial buildings are defined in terms of a mean scattering cross section and absorption coefficient are the most accurate. At the present time there exists no method of determining these parameters. From consideration of the behaviour of sound in a proportionate live room (reverberation chamber) it is shown that the scatterers with a low mean coefficient of absorption the product of mean scattering cross section and absorption coefficient is equal to one quarter of the effective area of absorption of the fitting. The results of computer simulation employing the RAYSCAT model suggest that, although individual values of the two parameters are required as input data, it is actually the product of the two parameters which determines the sound propagation characteristics of a room containing scattering fittings. The results obtained from further simulations suggest that if the equivalent area of absorption of fittings is known, then the sound propagation characteristics of a room containing those fittings can be predicted to a high degree of accuracy by employing an estimated a value of mean absorption coefficient and a value of mean scattering cross section calculated as equal to the effective area of absorption divided by four times the estimated value of the absorption coefficient. In the companion paper which is to follow, the validity of these hypotheses is examined by means of measurements made on acoustic scale models.


Author(s):  
M. K. Lamvik ◽  
A. V. Crewe

If a molecule or atom of material has molecular weight A, the number density of such units is given by n=Nρ/A, where N is Avogadro's number and ρ is the mass density of the material. The amount of scattering from each unit can be written by assigning an imaginary cross-sectional area σ to each unit. If the current I0 is incident on a thin slice of material of thickness z and the current I remains unscattered, then the scattering cross-section σ is defined by I=IOnσz. For a specimen that is not thin, the definition must be applied to each imaginary thin slice and the result I/I0 =exp(-nσz) is obtained by integrating over the whole thickness. It is useful to separate the variable mass-thickness w=ρz from the other factors to yield I/I0 =exp(-sw), where s=Nσ/A is the scattering cross-section per unit mass.


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