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
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