Digital Signal Processing Reference
In-Depth Information
10
5
0
10
5
0
5
10
15
20
25
30
5
10
15
20
25
30
0 . 5 1 . 0 1 . 5 2 . 0 2 . 5 3 . 0 3 . 5 4 . 0
0
0
0 . 5 1 . 0 1 . 5 2 . 0 2 . 5 3 . 0 3 . 5 4 . 0
F (kHz)
F (kHz)
( a)
( b )
10
5
0
10
5
0
5
10
15
20
25
30
5
10
15
20
25
30
0
0 . 5 1 . 0 1 . 5 2 . 0 2 . 5 3 . 0 3 . 5 4 . 0
0
0 . 5 1 . 0 1 . 5 2 . 0 2 . 5 3 . 0 3 . 5 4 . 0
F (kHz)
F (kHz)
(c)
(d)
FIG. 4.28 The directivity factor of the second-order cardioid with one distinct null, as a
function of frequency, for different values of Δ : (a) Δ = 1 cm, (b) Δ = 2 cm, (c) Δ = 3 cm,
and (d) Δ = 5 cm.
D DN,2 ( ω )= 772
49
576
49 cos( ωτ 0 / 2) 18
7 cos(2 ωτ 0 )+ 32
7 cos(3 ωτ 0 / 2)
18
7 + 32
+ sinc ( ωτ 0 )cos( ωτ 0 )
7 cos( ωτ 0 / 2)
520
49 cos( ωτ 0 )+ 160
49 cos( ωτ 0 / 2) 288
sinc ( ωτ 0 )
49 cos(3 ωτ 0 / 2)
.
(4.47)
In Fig. 4.28, we plot G DN,2 [ h
( ω )] from (4.46), as a function of frequency, for
different values of δ .
Finally, to end this section, we give the gain for a point noise source:
2
2
16
7
16
1 − e 2 ωτ 0
7 e ωτ 0 / 2
G
NS,2 [ h
( ω )] =
,
(4.48)
D NS,2 ( ω )
where
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