mc33411a Freescale Semiconductor, Inc, mc33411a Datasheet - Page 31

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mc33411a

Manufacturer Part Number
mc33411a
Description
900 Mhz Analog Cordless Phone Baseband With Compander
Manufacturer
Freescale Semiconductor, Inc
Datasheet
Loop Filter Characteristics
fundamental loop characteristics, such as capture range,
loop bandwidth, lock–up time, and transient response are
controlled externally by loop filtering.
(PLL).
represented as follows:
800 µA/4π. More details about performance of different type
PLL loops, refer to Motorola application note AN535.
A current output, type 2 filter will be used in this discussion
since it has the advantage of improved step response,
velocity, and acceleration.
follows:
integrator, providing the type 2 response, and filters the
discrete current steps from the phase detector output. The
function of the additional components R2 and C2 is to create
a pole and a zero (together with C1) around the 0 dB point of
the open loop gain. This will create sufficient phase margin
for stable loop operation.
displayed in the form of a Bode plot. Since there are two
integrating functions in the loop, originating from the loopfilter
and the VCO gain, the open loop gain response follows a
second order slope (–40 dB/dec) creating a phase of –180
degrees at the lower and higher frequencies. The filter
characteristic needs to be determined such that it is adding a
fi
MOTOROLA RF/IF DEVICE DATA
Let’s consider the following discussion on loop filters. The
Figure 46 is the general model for a Phase Lock Loop
Where:
From control theory the loop transfer function can be
K pd can be either expressed as being 200 µA/4π or
The loop filter can take the form of a simple low pass filter.
The type 2 low pass filter discussed here is represented as
From Figure 47, capacitor C1 forms an additional
In Figure 48, the open loop gain and the phase is
Detector (K pd )
Phase
K pd = Phase Detector Gain Constant
K f = Loop Filter Transfer Function
K o = VCO Gain Constant
K n = Divide Ratio (N)
fi = Input frequency
fo = Output frequency
fo/N = Feedback frequency divided by N
with Additional Integrating Element
A
K
Figure 47. Loop Filter
From
Phase
Detector
Figure 46. PLL Model
pd
K n
K
Divider
Filter
f
(K n )
(K f )
K o
C1
Open loop gain
R2
C2
VCO
(K o )
To VCO
MC33411A/B
fo
pole and a zero around the 0 dB point to guarantee sufficient
phase margin in this design (Qp in Figure 48).
expressed as:
the Bode plot can now be defined as:
zero in order to assure maximum phase margin occurs at ω p
(see also Figure 48). This provides an expression for ω p :
The open loop gain including the filter response can be
The two time constants creating the pole and the zero in
By substituting equation (5) into (4), it follows:
The phase margin (phase + 180) is thus determined by:
At ω=ω p , the derivative of the phase margin may be set to
Or rewritten:
By substituting into equation (7), solve for T2:
0
A
openloop
Open Loop Gain
A
openloop
dQ p
Q p
d
T1
w
Figure 48. Bode Plot of Gain and
Phase in Open Loop Condition
+
+
+
arctan(
C1
R2C1C2
0
T2
j
+
+
w
w
K n j
+
T1
+
1
C2
K
w
w
w
tan
pd
K
T2)–arctan(
+
w
2 C1K
p
Phase
T2
(
pd
K o (1
w
+
w
1
T2)
K o T1
p
Q p
2
w
1
2 T2
n T2
T2T1
p
2
1
ω p
T2
j
w
j
1
4
w
Q p
w
+
R2C1C2
(R2C2)
C1 C2
T1)
1
1
T1
(
R2C2
w
T1)
j
j
w
w
)
T2
T1
2
–90
–180
(10)
31
(11)
(4)
(5)
(6)
(7)
(8)
(9)
0

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