Building Acoustics

(Ron) #1

268 Building acoustics


inside a subsystem. Implicitly; all quantities E, n and W are functions of frequency and
generally we shall use the angular frequency ω in the equations.
A simple practical example is depicted in Figure 7.3, a freely suspended plate
forced into vibrations by the sound field set up in the room by a loudspeaker. In section
7.3.1 below we shall apply the equations, which follow from the assumptions above, to
calculate the amount of vibration resulting from a given input power to the room.

1 2

diss
W 1
diss
W 2

in
W 1
in
W 2
'
W 12

'
W 21

1 2

diss
W 1
diss
W 2

in
W 1
in
W 2
'
W 12

'
W 21

E 11 n E 22 n


Figure 7.2 System with two components (subsystems).

W


V
S

Figure 7.3 Example of a system with two components; a room being the acoustic component having volume V
and a free hanging panel of area S as the solid structure.


Assumption no. 1 above gives


WaEdiss= ⋅ , (7.1)


where a is factor of proportionality. As shown earlier (see section 6.4.1), we found for a
plate, having an area S and a mass m per unit area, that the relationship between the its
mean square velocity and mechanical power W was given by


WmS u^2 E,
ω


ωη ωη
Δ

=⋅ = (7.2)

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