Digital Signal Processing Reference
In-Depth Information
¼
/
ð
k
Þ
/
ð
k
þ
1
Þ
u
k
v
k
x
k
¼
Then, using Eq.
3.40
one has:
¼
u
k
þ
1
v
k
þ
1
/
ð
k
þ
1
Þ
/
ð
k
þ
2
Þ
x
k
þ
1
¼
¼
¼
g
ð
x
k
Þ
v
k
2v
k
u
k
þ
K
2
sin
ð
u
k
Þ
rK
2
sin
ð
v
k
Þ
f
ð
x
k
Þ
h
ð
x
k
Þ
¼
The problem is now expressed in a form which can be analyzed with fixed point
analysis:
and
;
u
v
g
ð
x
Þ¼
f
ð
x
Þ
h
ð
x
Þ
g(x) = x
with
x
¼
where
f(x) = v
and
h
ð
x
Þ¼
2v
u
þ
K
2
sin
ð
u
Þ
rK
2
sin
ð
v
Þ:
As there is a function of two variables, one should use the Jacobian (instead of
the derivative):
g
0
ð
x
Þ¼
of
=
ou
¼
of
=
ov
0
1
oh
=
ou
oh
=
ov
1
þ
K
2
cos
ð
u
Þ
2
rK
2
cos
ð
v
Þ
v
¼
ð
mod 2p
Þ
, at which:
u
0
0
The fixed point is x
¼
:
0
1
g
0
ð
x
Þ¼
1
þ
K
2
2
rK
2
For this system to have a fixed point as above, one should have:
j
k
i
j
\1
8
i
(x
*
), i.e., roots of |k I - L| = 0. Hence we
where k
i
are the eigenvalues of L = g
0
get:
r [ 1
and
4
r
þ
1
0\K
2
\
which define the locking range of SDPLL2.
3.4.2.5 PM Demodulation Using the SDPLL
Using Eq.
3.29
for the 1st-order SDPLL yields:
/
ð
k
Þ¼
h
ð
k
Þ
x
0
X
y
ð
i
Þ¼
h
ð
k
Þ
K
1
X
k
1
k
1
sin
½
/
ð
i
Þ
ð
3
:
41
Þ
i
¼
0
i
¼
0
Search WWH ::
Custom Search