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Digital PLL Synthesis
Digital PLL Synthesis
National Semiconductor
Application Note 335
Craig Davis
Tom Mills
Keith Mueller
April 1983
I. System Concepts
INTRODUCTION
Digital tuning systems are fast replacing the conventional
mechanical systems in AM/FM and television receivers.
The desirability of the digital approach is mainly due to the
following features:
Y Precise tuning of station frequencies
Y Exact digital frequency display
Y Keyboard entry of desired frequency
Y Virtually unlimited station memory
Y Up/down scanning through the band
Y Station ``search'' (stop on next active station)
Y Power on to the last station
Y Easy option for time-of-day clock
In addition, recent developments in large scale integrated
circuit technology and new varactor diodes for the AM band
have made the cost-benefit picture for digital tuning very
attractive. System partitioning is extremely important in opti-
mizing this cost-benefit picture, as will be discussed.
SYSTEM DESCRIPTION
A simplified block diagram of a typical digitally tuned receiv-
er is shown inFigure1. Notice this receiver could be one for
AM, FM, marine radio, or television; it makes no difference.
The frequency synthesizer block generates the local oscilla-
tor frequency for the receiver, just as a conventional me-
chanical tuner would. However, the phase-locked-loop
(PLL) acts as an integral frequency multiplier of an accurate
crystal controlled reference frequency while the mechanical
type provides a continuously variable frequency output with
no reference. Some method of controlling the value of the
multiplier for channel tuning must be provided. The other
RF, IF, and audio/video circuitry will be the same as in the
mechanical tuning method.
There are many different ways to partition the frequency
synthesizer system to perform the digital tuning function.
TL/F/5269±1
FIGURE 1. Block Diagram of a Digitally Tuned Receiver
COPS TM is a trademark of National Semiconductor Corp.
C 1995 National Semiconductor Corporation
TL/F/5269
RRD-B30M105/Printed in U. S. A.
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PROGRAMMABLE CONTROLLER FUNCTION
The most cost-effective application of different IC process
technologies is shown inFigure2. The controller is separate
from the PLL. The controller can be as simple as a mask
programmable microcontroller* or as complicated as a high-
powered microprocessor system. It can be done most eco-
nomically with NMOS technology because of the logic den-
sity possible and the small size of the RAM/ROM memory
cells. It could also be CMOS for extremely low power con-
sumption in standby mode.
BASIC PHASE-LOCKED-LOOP FUNCTION
The DS8906/7/8 series of PLLs utilize a dual-modulus fre-
quency synthesis technique. The reasons for this and the
PLL itself will now be discussed.
Figure3 is a diagram of the most simple phase-locked-loop.
A particular reference frequency is generated by a crystal
oscillator and some fixed divider, and this goes into one side
*Such as National's COP TM family.
of a digital phase comparator. A voltage controlled oscillator
(VCO) feeds directly into the other input of the phase com-
parator. The output of the phase comparator is an error sig-
nal which is filtered and fed back to the VCO as a DC con-
trol voltage.
In lock, the phase error must be zero, so f IN equals f REF .
This system provides only one output frequency, that being
equal to the reference frequency.
Figure4 is basically the same but now a programmable di-
vide-by-N counter is between the VCO and the phase com-
parator. The input to the phase comparator (f IN ) now be-
comes the output frequency of the VCO (f OUT ) divided by N,
where N is the division code loaded into the programmable
counter. This means f OUT /N must equal f REF . Thus, the
VCO output frequency becomes N c f REF , and f OUT can
now be changed in integral steps of f REF by merely chang-
ing N.
TL/F/5269±2
FIGURE 2. System Block Diagram
f IN e f REF
TL/F/5269±3
FIGURE 3. Basic Phase-Locked-Loop
f IN e f REF
f IN e
f OUT
N e f REF
f OUT e N c t REF x f STEP
e f REF
TL/F/5269±4
FIGURE 4. Basic PLL Frequency Synthesizer
2
f OUT
N
383702421.009.png
 
In applications where the output frequency desired exceeds
the maximum clock frequency of available programmable
dividers, a common solution is to add a prescaler preceding
the programmable divider, as shown inFigure5. In this case
f OUT e N(M c f REF ) and so the output frequency step size
becomes M c f REF . So, while this technique allows higher
frequency operation, it does so at the expense of either
increased channel spacing for a given reference frequency,
or decreased reference frequency if a specific channel
spacing is required. This latter limitation is often undesirable
as it can cause increased lock-on time, decreased scanning
rates, and sidebands at undesirable frequencies.
Figure 6 shows the basic dual-modulus scheme. Here, a
dual-modulus prescaler is substituted for the fixed prescaler
and the modulus is controlled by programmable counters.
The advantage to this approach is that the step size is again
equal to the reference frequency while the prescaling still
allows the programmable counters to operate at lower fre-
quencies. As in the fixed prescale technique, only the pre-
scaler needs to be high speed. The DS8906/7/8 prescale
by 7/8 for AM and in a similar fashion by 63/64 in FM.
f IN e f REF
f IN e
f OUT
N c M
FIGURE 5. PLL Frequency Synthesizer with Fixed Prescaler
f OUT
N c M e f REF
f OUT e (N c M) f REF
TL/F/5269±5 f OUT e N(M c f REF )
x f STEP e M c f REF
f OUT
N e f REF
f OUT e N c f REF x f STEP e f REF
*if f REF e f IN , then ``tuned''
if f REF i f IN , then ``not tuned''
f IN e
TL/F/5269±6
FIGURE 6. Basic Dual-Modulus Frequency Synthesizer
3
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II. Application Hints
VOLTAGE CONTROLLED OSCILLATORS
In all radio and television applications, the voltage con-
trolled oscillator (VCO) is a varactor tuned, LC type of cir-
cuit. The LC circuit is used over the various RC current con-
trolled circuits because of their superior noise characteris-
tics. Figure7 shows a collection of popular VCOs used in
radio and television tuners. The AM VCO is a Hartley design
chosen for wide tuning range. Commonly used varactors will
show a capacitance change of 350 pF at 1V to 20 pF at 8V,
which if used in a low capacitance oscillator circuit, can pro-
duce a tuning range approaching 3 to 1.
In the higher frequency ranges, above 50 MHz, Colpitts os-
cillators are used because stray circuit capacitance will be in
parallel with desired feedback capacitance and not cause
undesirable spurious resonances that might occur with the
tapped coil Hartley design. The FM VCO shown is a ground-
ed base design with feedback from collector to emitter. A
UHF television oscillator is also shown. It too is a grounded
base oscillator, but using a transmission line as the reso-
nant element instead of a coil. The transmission line and
tuning capacitors are arranged in q network which offers
improved noise characteristics over a parallel tuned circuit.
This circuit will tune over almost an octave.
Hartley Oscillator
TL/F/5269±7
50 kHz E 15 MHz VCO
Tuning range j 3:1
Colpitts Oscillator
Colpitts Oscillator
TL/F/5269±8
50 MHz E 300 MHz VCO
Tuning range j 2:1
TL/F/5269±9
500 MHz E 1000 MHz VCO
Tuning range j 1.8:1
FIGURE 7. Typical VCO Circuits (Typical Values Shown)
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PLL LOOP FILTER CALCULATIONS
Andrzej Przedpelski, in two articles published in Electronic
Design ( Ý 19, Sept. 13, 1978 and Ý 10, May 10, 1978) ex-
plains how to calculate the three time constants associated
with a third order type 2 loop which is typically used with the
DS8906/7/8 series. Figure 8 explains his method and
shows a sample calculation. His articles illustrate how to
calculate three time constants, and plot open loop gain and
phase, and closed loop noise response.
It should be noted that VCO gain, K V , is in terms of radians
per second per volt, and phase detector gain, K D , is in terms
of amps per radian. The phase detector gain for the
DS8906/7/8 series is g I OUT divided by 4 q .
Figure 9 illustrates an example calculation of time con-
stants, and a plot of open loop gain and phase based on the
preceding analysis.
REFERENCES
1. Manassewitsch V., ``Frequency Synthesizers'' (Wiley,
New York, 1976)
2. Rohde, A. L., ``Digital PLL Frequency Synthesizers''
(Prentice Hall, Englewood Cliffs, 1983)
3. Egan, W. F., ``FrequencySynthesisByPhaseLock'' (Wi-
ley, New York, 1981)
T1 e R1C1
T1 e R1C2
eV
I O
e
1 a ST1
SC1 (1 a ST2)
G(S) e
K D K V
NS 2 C1
#
1 a ST1
1 a ST2
J
T2 e
1 b tan w cos w
0 O cos w
T1 e
1
0 O 2 T2
J
where i e desired phase margin
0 O e loop natural frequency
& closed loop bandwidth
Note: DS8909 op amp required C3 & 1000 pF for compensation.
FIGURE 8. Third Order Type 2 Loop
C1 e
K D K V
N 0 O 2
#
b 0 O T1 b 1
0 O T2 a 1
TL/F/5269±10
VHF loop, running at 100 MHz, ref e 10 kHz
K V e 2.5 MHz/V e 15.7 Mrad/sec/V
K D e
400 m A
4 q
e 31.8 m A/radian
100 MHz
10 kHz e 10,000, 0 O e 2 q c 100 Hz
i e 45 § (desired phase margin)
T2 e 6.6 c 10 b 4 sec
T1 e 3.84 c 10 b 3 sec
C1 e 0.3 m F
so R1 e T1/C1 e 13 k X
C2 e T2/R1 e 0.05 m F
TL/F/5269±11
FIGURE 9. Example of Gain and Phase Calculation
5
N e
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