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IEEE SIGNAL PROCESSING MAGAZINE [87] MARCH 2015
infinite norm. Equation (12) can be solved analytically for the
pp2
ud
==
case where it reduces to a generalized Rayleigh quo-
tient. In general, (12) is solved using the steepest descent meth-
ods [25]. A relaxed multichannel approach using least squares
[26] and minimax metrics [24] may include regularizations to
reduce the array effort below that of the ratio-based approach in
[25]. These approaches are compared in Figure 5 for simulation
with
L 3= and Q 2= in a room with a reverberation time of
250 ms using only 150 ms-long reshaping filters. The ratio-based
approach shown is for
,p 10
u
= ,p 01
d
= and 1,000 steepest
descent iterations.
Impulse response reshaping, in principle, can be applied to
the PM- and modal-space approaches of creating personal sound
zones. More robust and efficient filters can be obtained than
equalization by canceling the undesirable late reverberation
while leaving in some beneficial early reflections. Unfortunately
this problem must be formulated in the time domain, which
results in a computationally intractable massive multichannel
problem. The future development of lower-complexity convex
optimization algorithms may permit practical solutions to these
large problems.
DIRECTIONAL SOURCES
The use of directional sources can provide advantages over con-
ventional loudspeakers, whose directivity is omnidirectional at low
frequencies and is not typically controllable. Directional sources
that provide multiple modes of sound radiation can be used with
active compensation to produce sound arriving from angles where
there are no sources by reflecting sound from room surfaces and
can also cancel unwanted reverberation (Figure 6).
In a multilistener situation, a single directional loudspeaker
can reduce unwanted radiation of sound to other listeners by max-
imizing the direct sound to the intended recipient relative to the
reverberant field. A loudspeaker with directivity
D and radiating
acoustic power W in an ideal Sabinian space produces a direct
sound intensity /( )I WDr4
2
dir
r= and a reverberant sound inten-
sity of /,I W R4
rev
=
l
where /( )RS1
ee=-
l
is the room con-
stant, S the room surface area, and
e
the mean absorption
coefficient of the room surfaces. The direct to reverberant inten-
sity ratio is thus
.
r
DR
4
DRR
2
r
=
l
(13)
Increasing the directivity then allows the direct sound at the lis-
tener to be increased relative to the reverberant sound. Equiva-
lently, the reverberant field is reduced by /.DRR1
100 200 300
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−10
0
Time (ms)
Magnitude (dB)
100 200 300
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−10
0
Time (ms)
Magnitude (dB)
100 200 300
−80
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−60
−50
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−10
0
Time (ms)
(a) (b)
(c)
Magnitude (dB)
Delivered
Crosstalk
[FIG5] The shortening of impulse responses to 50 ms in a room of reverberation time 250 ms using (a) relaxed multichannel least
squares, (b) the relaxed minimax approach in [24], and (c) the ratio optimization approach of [25].
Room
Walls
Zone
Reflections
r
Higher-Order
Loudspeaker
(a)
(b)
[FIG6]
A demonstration of the higher-order loudspeaker in (a) a
cylindrical baffle and (b) the schematic plot of its behavior.
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