Sound absorbers 189
125 250 500 1000 2000 4000
Frequency (Hz)
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
1.1
1.2
1.3
1.4
1.5
Abso
rption
facto
r
Distance x in cm
0
20
40
60
80
100
1.20
0.60
x x
Figure 5.25 Reverberation room measurements of the absorption factor of eight mineral wool blankets, 25 mm
thick and having a total area of 5.8 m^2. Dimensions and measured configuration is shown in the sketch. Student
tutorial, NTNU.
5.5.4 Further models for materials with a stiff frame (skeleton)
In more recent years there has been development of several models using a more detailed
description of the structure of the material, the aim being to use directly measurable
material quantities. Early work on this (e.g. Zwikker and Kosten (1949)), introduced a
structure factor in addition to the flow resistivity and porosity, a factor that is now
termed tortuosity or sinuosity. In a popular way, we may say that this parameter gives us
information on the directionality of the pores in the material. In a material having straight
through pores of cylindrical shape making an angle φ with the outer surface, the
tortuosity ks is given by
(^) s 2
1
,
cos
k
φ
= (5.59)
which, as an example, gives ks equals 2 for φ equal 45°. In many applications however, a
model using these three parameters will be too simple even for materials where one
assumes isotropy and a stiff frame.