MC74HC4046A
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7
DETAILED CIRCUIT DESCRIPTION
Voltage Controlled Oscillator/Demodulator Output
The VCO requires two or three external components to
operate. These are R1, R2, C1. Resistor R1 and Capacitor C1
are selected to determine the center frequency of the VCO
(see typical performance curves Figure 15). R2 can be used
to set the offset frequency with 0 volts at VCO input. For
example, if R2 is decreased, the offset frequency is
increased. If R2 is omitted the VCO range is from 0 Hz. The
effect of R2 is shown in Figure 25, typical performance
curves. By increasing the value of R2 the lock range of the
PLL is increased and the gain (volts/Hz) is decreased. Thus,
for a narrow lock range, large swings on the VCO input will
cause less frequency variation.
Internally, the resistors set a current in a current mirror, as
shown in Figure 6. The mirrored current drives one side of
the capacitor. Once the voltage across the capacitor charges
up to V
ref
of the comparators, the oscillator logic flips the
capacitor which causes the mirror to charge the opposite side
of the capacitor. The output from the internal logic is then
taken to VCO output (Pin 4).
The input to the VCO is a very high impedance CMOS
input and thus will not load down the loop filter, easing the
filters design. In order to make signals at the VCO input
accessible without degrading the loop performance, the
VCO input voltage is buffered through a unity gain Op−amp
to Demod Output. This Op−amp can drive loads of 50K
ohms or more and provides no loading effects to the VCO
input voltage (see Figure 13).
An inhibit input is provided to allow disabling of the VCO
and all Op−amps (see Figure 6). This is useful if the internal
VCO is not being used. A logic high on inhibit disables the
VCO and all Op−amps, minimizing standby power
consumption.
Figure 6. Logic Diagram for VCO
_
+
_
+
_
+
I
1
I
2
R
2
12
V
REF
VCO
IN
R
1
9
11
10
5
6
7
4
++
V
ref
C
1
(EXTERNAL)
DEMOD
OUT
CURRENT
MIRROR
I
1
+ I
2
= I
3
VCO
OUT
INH
I
3
The output of the VCO is a standard high speed CMOS
output with an equivalent LS−TTL fan out of 10. The VCO
output is approximately a square wave. This output can
either directly feed the COMP
IN
of the phase comparators or
feed external prescalers (counters) to enable frequency
synthesis.
MC74HC4046A
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Phase Comparators
All three phase comparators have two inputs, SIG
IN
and
COMP
IN
. The SIG
IN
and COMP
IN
have a special DC bias
network that enables AC coupling of input signals. If the
signals are not AC coupled, standard 74HC input levels are
required. Both input structures are shown in Figure 7. The
outputs of these comparators are essentially standard 74HC
outputs (comparator 2 is TRI−STATEABLE). In normal
operation V
CC
and ground voltage levels are fed to the loop
filter. This differs from some phase detectors which supply
a current to the loop filter and should be considered in the
design. (The MC14046 also provides a voltage).
Figure 7. Logic Diagram for Phase Comparators
SIG
IN
COMP
IN
V
CC
V
CC
V
CC
14
3
13
1
15
2
PC2
OUT
PCP
OUT
PC3
OUT
PC1
OUT
Phase Comparator 1
This comparator is a simple XOR gate similar to the
74HC86. Its operation is similar to an overdriven balanced
modulator. To maximize lock range the input frequencies
must have a 50% duty cycle. Typical input and output
waveforms are shown in Figure 8. The output of the phase
detector feeds the loop filter which averages the output
voltage. The frequency range upon which the PLL will lock
onto if initially out of lock is defined as the capture range.
The capture range for phase detector 1 is dependent on the
loop filter design. The capture range can be as large as the
lock range, which is equal to the VCO frequency range.
To see how the detector operates, refer to Figure 8. When
two square wave signals are applied to this comparator, an
output waveform (whose duty cycle is dependent on the
phase difference between the two signals) results. As the
phase difference increases, the output duty cycle increases
and the voltage after the loop filter increases. In order to
achieve lock when the PLL input frequency increases, the
VCO input voltage must increase and the phase difference
between COMP
IN
and SIG
IN
will increase. At an input
frequency equal to f
min
, the VCO input is at 0 V. This
requires the phase detector output to be grounded; hence, the
two input signals must be in phase. When the input
frequency is f
max
, the VCO input must be V
CC
and the phase
detector inputs must be 180 degrees out of phase.
Figure 8. Typical Waveforms for PLL Using
Phase Comparator 1
V
CC
GND
SIG
IN
COMP
IN
PC1
OUT
VCO
IN
The XOR is more susceptible to locking onto harmonics
of the SIG
IN
than the digital phase detector 2. For instance,
a signal 2 times the VCO frequency results in the same
output duty cycle as a signal equal to the VCO frequency.
The difference is that the output frequency of the 2f example
is twice that of the other example. The loop filter and VCO
range should be designed to prevent locking on to
harmonics.
MC74HC4046A
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Phase Comparator 2
This detector is a digital memory network. It consists of
four flip−flops and some gating logic, a three state output
and a phase pulse output as shown in Figure 6. This
comparator acts only on the positive edges of the input
signals and is independent of duty cycle.
Phase comparator 2 operates in such a way as to force the
PLL into lock with 0 phase difference between the VCO
output and the signal input positive waveform edges. Figure
8 shows some typical loop waveforms. First assume that
SIG
IN
is leading the COMP
IN
. This means that the VCO’s
frequency must be increased to bring its leading edge into
proper phase alignment. Thus the phase detector 2 output is
set high. This will cause the loop filter to charge up the VCO
input, increasing the VCO frequency. Once the leading edge
of the COMP
IN
is detected, the output goes TRI−STATE
holding the VCO input at the loop filter voltage. If the VCO
still lags the SIG
IN
then the phase detector will again charge
up the VCO input for the time between the leading edges of
both waveforms.
If the VCO leads the SIG
IN
then when the leading edge of
the VCO is seen; the output of the phase comparator goes
low. This discharges the loop filter until the leading edge of
the SIG
IN
is detected at which time the output disables itself
again. This has the effect of slowing down the VCO to again
make the rising edges of both waveforms coincidental.
When the PLL is out of lock, the VCO will be running
either slower or faster than the SIG
IN
. If it is running slower
the phase detector will see more SIG
IN
rising edges and so
the output of the phase comparator will be high a majority
of the time, raising the VCO’s frequency. Conversely, if the
VCO is running faster than the SIG
IN
, the output of the
detector will be low most of the time and the VCO’s output
frequency will be decreased.
As one can see, when the PLL is locked, the output of
phase comparator 2 will be disabled except for minor
corrections at the leading edge of the waveforms. When PC
2
is TRI−STATED, the PCP output is high. This output can be
used to determine when the PLL is in the locked condition.
This detector has several interesting characteristics. Over
the entire VCO frequency range there is no phase difference
between the COMP
IN
and the SIG
IN
. The lock range of the
PLL is the same as the capture range. Minimal power was
consumed in the loop filter since in lock the detector output
is a high impedance. When no SIG
IN
is present, the detector
will see only VCO leading edges, so the comparator output
will stay low, forcing the VCO to f
min
.
Phase comparator 2 is more susceptible to noise, causing
the PLL to unlock. If a noise pulse is seen on the SIG
IN
, the
comparator treats it as another positive edge of the SIG
IN
and will cause the output to go high until the VCO leading
edge is seen, potentially for an entire SIG
IN
period. This
would cause the VCO to speed up during that time. When
using PC
1
, the output of that phase detector would be
disturbed for only the short duration of the noise spike and
would cause less upset.
Phase Comparator 3
This is a positive edge−triggered sequential phase
detector using an RS flip−flop as shown in Figure 7. When
the PLL is using this comparator, the loop is controlled by
positive signal transitions and the duty factors of SIG
IN
and
COMP
IN
are not important. It has some similar
characteristics to the edge sensitive comparator. To see how
this detector works, assume input pulses are applied to the
SIG
IN
and COMP
IN
’s as shown in Figure 10. When the
SIG
IN
leads the COMP
IN
, the flop is set. This will charge the
loop filter and cause the VCO to speed up, bringing the
comparator into phase with the SIG
IN
. The phase angle
between SIG
IN
and COMP
IN
varies from 0° to 360° and is
180° at f
o
. The voltage swing for PC
3
is greater than for PC
2
but consequently has more ripple in the signal to the VCO.
When no SIG
IN
is present the VCO will be forced to f
max
as
opposed to f
min
when PC
2
is used.
The operating characteristics of all three phase
comparators should be compared to the requirements of the
system design and the appropriate one should be used.
Figure 9. Typical Waveforms for PLL Using
Phase Comparator 2
V
CC
GND
SIG
IN
COMP
IN
PC2
OUT
VCO
IN
PCP
OUT
HIGH IMPEDANCE OFF−STATE
Figure 10. Typical Waveform for PLL Using
Phase Comparator 3
VCC
GND
SIG
IN
COMP
IN
PC3
OUT
VCO
IN

MC74HC4046AFELG

Mfr. #:
Manufacturer:
ON Semiconductor
Description:
Phase Locked Loops - PLL LOG CMOS PLL
Lifecycle:
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