Civil Engineering Reference
In-Depth Information
6 and 9 dB higher than the average level in the room. This is also easily demonstrated by
direct measurements. Restricting the determination of the average sound pressure level to
the inner part of a room, normally half a wavelength away from the boundaries, implies
that we are “losing” a part of the sound energy. One therefore finds that the standards
include a frequency-dependent correction term, the so-called
Waterhouse correction
to
compensate for this effect and the power is then calculated from
2
p
⎛
Sc
⎞
⎟
∞
0
W
=
A
1
+
,
(4.31)
⎝
4
ρ
c
8
Vf
⎠
00
where
S
is the total surface area of the room. In addition, the standard ISO 3741 includes
some minor corrections for the barometric pressure and temperature and furthermore, the
absorption area
A
is substituted by the so-called
room constant R
where
A
A
R
=
=
,
(4.32)
A
S
1
−
α
1
−
and where
α
is the mean absorption factor of the room boundaries. Normally, the mean
absorption factor is required to be small for laboratory reverberation rooms making this
correction also small. However, in the high frequency range (above 8-10 kHz) this may
not be the case, especially due to air absorption (see section
4.5.1.3
).
4.5.1.2
Reverberation time
Turning off the sound source when the stationary condition is reached, i.e. setting
2
()
at time
t
= 0, and
W
= 0 for
t
> 0, we get
2
p
t
=
∞
Ac
0
−
⋅
t
2
2
pt
()
=⋅
p
e
4
V
.
(4.33)
As the reverberation time
T
is defined by the time elapsed for the sound pressure level to
decrease by 60 dB, or equivalent, that the sound energy density has decreased by a factor
10
-6
, we write
Ac
2
pT
p
()
0
−⋅
T
−
6
=
10
=
e
4
V
,
(4.34)
2
∞
which gives us the reverberation time, commonly denoted
T
60
, as
4 . 6
V
⋅
V
( )
6
T
=
ln 10
⋅
≈
.
(4.35)
60
cA
c
A
0
0
This is the famous reverberation time formula by Sabine, which is the most commonly
used in practice in spite of its simplicity and the assumptions lying behind its derivation.
Obviously, it cannot be applied for rooms having a very high absorption area. Setting the
absorption factor equal to 1.0 for all surfaces, we still get a finite reverberation time
whereas it is obvious that we shall get no reverberation at all. Other formulae have been
