Digital Signal Processing Reference
In-Depth Information
where
d i is the projected element distance and
is the angular rotation of the
elements.
x i ð
t
Þ¼
sin 2
½
ft
þ ' i
:
ð
6
:
2
Þ
The phase detector output m 1 ð
t
Þ
is obtained from r
ð
t
Þ¼
sin
ð
2
ft
Þ
and x i ð
t
Þ
:
h
ð
i
cos
m 1 ð
Þ¼
ð' i Þ¼
Þ
ð
Þ
:
ð
:
Þ
t
cos
D cos
i
cos
t
6
3
Signal m 1 ð t Þ
is passed through an FM discriminator and another phase detector,
giving
x
~
ð
t
Þ¼
A x cos
ð
t
þ 1 ð
t
ÞÞ;
ð
6
:
4
Þ
~
y
ð
t
Þ¼
A y cos
ð
t
þ 2 ð
t
ÞÞ;
ð
6
:
5
Þ
where A x ¼
K y is zero in a least-squares
sense for a given system. Traditional analogue systems present DoA by inputting
~
K x cos
ðÞ
, A y ¼
K y sin
ðÞ
and e
¼
K x
x
ð
t
Þ
and
y
~
ð
t
Þ
to an X-Y scope, shown in Figure 6.4(a). The phase distortions
1 ð
t
Þ
and
are the undesired phase modulations due to multiple reflections,
instrumentation errors, etc., and the plot between
2 ð
t
Þ
x
~
ð
t
Þ
and
y
~
ð
t
Þ
results in a
distorted figure of eight. The ratio between the amplitudes of
Þ
has the DoA information in it and the sinusoids are in phase with each other.
However, finding a direct ratio is catastrophic and here we formulate it as a
DSP problem.
x
~
ð
t
Þ
and
y
~
ð
t
1
1
0.5
0.5
0
0
−0.5
−0.5
1
−1
0.5
0
0.5
−0.5
0
0.5
Digital
Analogue
(b)
(a)
Figure 6.4 DOA using DSP in a rotary system
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