MPC9229
TIMING SOLUTIONS 7 MOTOROLA
Substituting N for the four available values for N (1, 2, 4, 8)
yields:
Table 8. Output Frequency Range for f
XTAL
=16MHz
N
F
OUT
F
OUT
range F
OUT
step
1 0 Value
O
U
O
U
g
O
U
p
0 0 1 M 200 - 400 MHz 1MHz
0 1 2 M÷2 100 - 200 MHz 500 kHz
1 0 4 M÷4 50 - 100 MHz 250 kHz
1 1 8 M÷8 25 - 50 MHz 125 kHz
Example frequency calculation for an 16 MHz input
frequency
If an output frequency of 131 MHz was desired the following
steps would be taken to identify the appropriate M and N
values. According to Table 8, 131 MHz falls in the frequency
set by an v alue of 2 so N[1:0] = 01. For N = 2 the output
frequency is F
OUT
=M÷ 2 and M = F
OUT
x 2. Therefore M =
2 x 131 = 262, so M[8:0] = 100000110. Following this
procedure a user can generate any whole frequency between
25 MHz and 400 MHz. Note than for N > 2 fractional values of
can be realized. The size of the programmable frequency
steps (and thus the indicator of the fractional output
frequencies achievable) will be equal to:
f
STEP
=f
XTAL
÷ 16 ÷ N(6)
Using the parallel and serial interface
The M and N counters can be loaded either through a
parallel or serial interface. The parallel interface is controlled
via the P_LOAD
signal such that a LOW to HIGH transition will
latch the information present on the M[8:0] and N[1:0] inputs
into the M and N counters. When the P_LOAD
signal is LOW
the input latches will be transparent and any changes on the
M[8:0] and N[1:0] inputs will affect the FOUT output pair. To
use the serial port the S_CLOCK signal samples the
information on the S_DATA line and loads it into a 14 bit shift
register. Note that the P_LOAD
signal must be HIGH for the
serial load operation to function. The Test register is loaded
with the first three bits, the N register with the next two and the
M register with the final eight bits of the data stream on the
S_DATA input. For each register the most significant bit is
loaded first (T2, N1 and M8). A pulse on the S_LOAD pin after
the shift register is fully loaded will transfer the divide values
into the counters. The HIGH to LOW transition on the S_LOAD
input will latch the new divide values into the counters. Figure
4 illustrates the timing diagram for both a parallel and a serial
load of the MPC9229 synthesizer. M[8:0] and N[1:0] are
normally specified once at power–up through the parallel
interface, and then possibly again through the serial interface.
This approach allows the application to come up at one
frequency and then change or fine–tune the clock as the ability
to control the serial interface becomes available.
Using the test and diagnosis output TEST
The TEST output provides visibility for one of the several
internal nodes as determined by the T[2:0] bits in the serial
configuration stream. It is not configurable through the parallel
interface. Although it is possible to select the node that
represents F
OUT
, the CMOS output is not able to toggle fast
enough for higher output frequencies and should only be used
for test and diagnosis. The T2, T1 and T0 control bits are
preset to ‘000’ when P_LOAD
is LOW so that the PECL FOUT
outputs are as jitter–free as possible. Any active signal on the
TEST output pin will have detrimental affects on the jitter of the
PECL output pair. In normal operations, jitter specifications are
only guaranteed if the TEST output is static. The serial
configuration port can be used to select one of the alternate
functions for this pin. Most of the signals available on the TEST
output pin are useful only for performance verification of the
MPC9229 itself. However the PLL bypass mode may be of
interest at the board level for functional debug. When T[2:0] is
set to 110 the MPC9229 is placed in PLL bypass mode. In this
mode the S_CLOCK input is fed directly into the M and N
dividers. The N divider drives the F
OUT
differential pair and the
M counter drives the TEST output pin. In this mode the
S_CLOCK input could be used for low speed board level
functional test or debug. Bypassing the PLL and driving F
OUT
directly gives the user more control on the test clocks sent
through the clock tree. Figure 6 shows the functional setup of
the PLL bypass mode. Because the S_CLOCK is a CMOS
level the input frequency is limited to 200 MHz. This means the
fastest the F
OUT
pin can be toggled via the S_CLOCK is 100
MHz as the divide ratio of the Post-PLL divider is 2 (if N = 1).
Note that the M counter output on the TEST output will not be
a 50% duty cycle.
Table 9. Test and Debug Configuration for TEST
T[2:0]
TEST output
T2 T1 T0
p
0 0 0 14-bit shift register out
a
0 0 1 Logic 1
0 1 0 f
XTAL
÷ 16
0 1 1 M-Counter out
1 0 0 FOUT
1 0 1 Logic 0
1 1 0 M-Counter out in PLL-bypass mode
1 1 1 FOUT ÷ 4
a. Clocked out at the rate of S_CLOCK
Table 10. Debug Configuration for PLL bypass
a
Output Configuration
F
OUT
S_CLOCK ÷ N
TEST M-Counter out
b
a. T[2:0]=1 10. AC specifications do not apply in PLL bypass
mode
b. clocked out at the rate of S_CLOCK÷(4N)
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MPC9229
MOTOROLA TIMING SOLUTIONS8
Figure 4. Serial Interface Timing Diagram
S_CLOCK
S_DATA
S_LOAD
M[8:0]
N[1:0]
P_LOAD
T2 T1 T0 N1 N0 M8 M7 M6 M5 M4 M3 M2 M1
M0
M, N
First
Bit
Last
Bit
Power Supply Filtering
The MPC9229 is a mixed analog/digital product. Its analog
circuitry is naturally susceptible to random noise, especially if
this noise is seen on the power supply pins. Random noise on
the VCC_PLL pin impacts the device characteristics. The
MPC9229 provides separate power supplies for the digital
circuitry (VCC) and the internal PLL (VCC_PLL) of the device.
The purpose of this design technique is to try and isolate the
high switching noise digital outputs from the relatively
sensitive internal analog phase–locked loop. In a controlled
environment such as an evaluation board, this level of
isolation is sufficient. However, in a digital system environment
where it is more difficult to minimize noise on the power
supplies a second level of isolation may be required. The
simplest form of isolation is a power supply filter on the
VCC_PLL pin for the MPC9229. Figure 5 illustrates a typical
power supply filterscheme. The MPC9229 is most susceptible
to noise with spectral content in the 1 kHz to 1 MHz range.
Therefore, the filter should be designed to target this range.
The key parameter that needs to be met in the final filter design
is the DC voltage drop that will be seen between the VCC
supply and the MPC9229 pin of the MPC9229. From the data
sheet, the VCC_PLL current (the current sourced through the
VCC_PLL pin) is maximum 20 mA, assuming that a minimum
of 2.835 V must be maintained on the VCC_PLL pin. The
resistor shown in Figure 5 must have a resistance of 10-15
to meet the voltage drop criteria. The RC filter pictured will
provide a broadband filter with approximately 100:1
attenuation for noise whose spectral content is above 20 kHz.
As the noise frequency crosses the series resonant point of an
individual capacitor its overall impedance begins to look
inductive and thus increases with increasing frequency. The
parallel capacitor combination shown ensures that a low
impedance path to ground exists for frequencies well above
the bandwidth of the PLL. Generally, the resistor/capacitor
filter will be cheaper, easier to implement and provide an
adequate level of supply filtering. A higher level of attenuation
can be achieved by replacing the resistor with an appropriate
valued inductor. A 1000 µH choke will show a significant
impedance at 10 kHz frequencies and above. Because of the
current draw and the voltage that must be maintained on the
VCC_PLL pin, a low DC resistance inductor is required (less
than 15 ).
Figure 5. V
CC PLL
Power Supply Filter
VCC_PLL
V
CC
MPC9229
C
1
,C
2
= 0.01...0.1 µF
V
CC
C
F
=22µF
R
F
=10--15
C
2
C
1
Layout Recommendations
The MPC9229 provides sub–nanosecond output edge
rates and thus a good power supply bypassing scheme is a
must. Figure 6 shows a representative board layout for the
MPC9229. There exists many different potential board layouts
and the one pictured is but one. The important aspect of the
layout in Figure 6 is the low impedance connections between
VCC and GND for the bypass capacitors. Combining good
quality general purpose chip capacitors with good PCB layout
techniques will produce effective capacitor resonances at
frequencies adequate to supply the instantaneous switching
current for the MPC9229 outputs. It is imperative that low
inductance chip capacitors are used; it is equally important
that the board layout does not introduce back all of the
inductance saved by using the leadless capacitors. Thin
interconnect traces between the capacitor and the power
plane should be avoided and multiple large v ias should be
used to tie the capacitors to the buried power planes. Fat
interconnect and large vias will help to minimize layout
induced inductance and thus maximize the series resonant
point of the bypass capacitors. Note the dotted lines circling
the crystal oscillator connection to the device. The oscillator is
a series resonant circuit and the voltage amplitude across the
crystal is relatively small. It is imperativ e that no actively
switching signals cross under the crystal as crosstalk energy
coupled to these lines could significantly impact the jitter of the
device. Special attention should be paid to the layout of the
crystal to ensure a stable, jitter free interface between the
crystal and the on–board oscillator. Although the MPC9229
has several design features to minimize the susceptibility to
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MPC9229
TIMING SOLUTIONS 9 MOTOROLA
power supply noise (isolated power and grounds and fully
differential PLL), there still may be applications in which overall
performance is being degraded due to system power supply
noise. The power supply filter and bypass schemes discussed
in this section should be adequate to eliminate power supply
noise related problems in most designs.
Figure 6. PCB Board Layout Recomme ndation for
the PLCC28 Package
C2
1
C
F
Xtal
C1 C1
=V
CC
=GND
=Via
Using the On--Board Crystal Oscillator
The MPC9229 features a fully integrated on --board crystal
oscillator to minimize system implementation costs. The
oscillator is a series resonant, multivibrator type design as
opposed to the more common parallel resonant oscillator
design. The series resonant design provides better stability
and eliminates the need for large on chip capacitors. The
oscillator is totally self contained so that the only external
component required is the crystal. As the oscillator is
somewhat sensitive to loading on its inputs the user is advised
to mount the crystal as close to the MPC9229 as possible to
avoid any board level parasitics. To facilitate co--location
surface mount crystals are recommended, but not required.
Because the series resonant design is affected by capacitive
loading on the xtal terminals loading variation introduced by
crystals from different vendors could be a potential issue. For
crystals with a higher shunt capacitance it may be required to
place a resistance across the terminals to suppress the third
harmonic. Although typically not required it is a good idea to
layout the PCB with the provision of adding this external
resistor. The resistor value will typically be between 500 and
1K.
The oscillator circ uit is a series resonant circ uit and thus for
optimum performance a series resonant crystal should be
used. Unfortunately most crystals are characterized in a
parallel resonant mode. Fortunately there is no physical
difference between a series resonant and a parallel resonant
crystal. The difference is purely in the way the devices are
characterized. As a result a parallel resonant crystal can be
used with the MPC9229 with only a minor error in the desired
frequency. A parallel resonant mode crystal used in a series
resonant circuit will exhibit a frequency of oscillation a few
hundred ppm lower than specified, a few hundred ppm
translates to k Hz inaccuracies. In a general computer
application this level of inaccuracy is immaterial. Table 11
below specifies the performance requirements of the crystals
to be used with the MPC9229.
Table 11. Recommended Crystal Specifications
Parameter Value
Crystal Cut Fundamental AT Cut
Resonance Series Resonance*
Frequency Tolerance ±75ppm at 25°C
Frequency/Temperature Stability ±150pm 0 to 70°C
Operating Range 0to70°C
Shunt Capacitance 5--7pF
Equivalent Series Resistance (ESR) 50 to 80
Correlation Drive Level 100µW
Aging 5ppm/Yr (First 3 Years)
* See accompanying text for series versus parallel resonant
discussion.
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MPC9229FN

Mfr. #:
Manufacturer:
NXP / Freescale
Description:
Phase Locked Loops - PLL 3.3V 400MHz Clock Generator
Lifecycle:
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