Technical Notes on using Analog Devices' DSP components and development tools
a
Using Third Overtone Crystals with the ADSP-218x DSP
Contributed by Larry Hurst August 8, 2002
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rd
OT crystal has a lower activity, (i.e.
For these reasons, extra care should be
rd
OT crystal oscillators
Note that there is often no indication,
rd
OT operation verses
rd
OT operation.
Introduction
DSPs frequently require an input clock
frequency (CLKIN) that is over 35MHz.
Unfortunately fundamental mode crystals over
35MHz are not popular and tend to be expensive
and fragile. Packaged clock oscillators cost
considerably more than a crystal so, for some
applications, using a 3
may be a sensible choice.
While the current trend is to incorporate
PLL frequency multiplication into the DSP,
using a low frequency input clock to generate
internal core clocks of several hundred MHz,
there are still occasions when it might be useful
to consider using a 3
This note discusses using readily
available 3
rd
overtone crystals, at frequencies
over 35MHz, with the ADSP-218x family of
rd
overtone (3
rd
OT crystal.
rd
OT) crystal
Second, a 3
requires a higher minimum drive level to start
reliably).
taken when designing 3
and careful testing should be performed over
temperature, voltage and with a representative
batch of crystals to ensure that all parts operate
reliably.
marked on the crystal package, to show that a
crystal is intended for 3
fundamental mode operation. Care should be
taken to determine this information. If a crystal
is used in a traditional (two capacitor
fundamental mode circuit) appears to be
oscillating at approximately one third of the
frequency marked on it’s package, it is very
likely that it is intended for 3
DSPs. A design procedure is developed for
calculating the optimum values for the support
components. This procedure can be extended to
CODECs and other applications requiring input
clocks over 35MHz.
Design Method
When a 3rd OT crystal is chosen, two
additional circuit components must
the traditional parallel, or fundamental mode
be added to
circuit, to force oscillation at the overtone
Cautionary Note
There are a number of cautions that
should be noted when deciding to use a 3
crystal oscillator.
First, a 3
rd
OT crystal normally has a
higher ESR, typically more than twice that of a
rd
OT
frequency marked on the crystal. The added
components consist of a series inductor and
capacitor as shown in Figure 1. If L
and C3 are
1
not added to the circuit, the crystal will oscillate
at its fundamental frequency, which is
approximately
one third of the desired overtone
frequency.
fundamental mode crystal at the same frequency.
Copyright 2002, Analog Devices, Inc. All rights reserved. Analog Devices assumes no responsibility for customer product design or the use or application of
customers’ products or for any infringements of patents or rights of others which may result from Analog Devices assistance. All trademarks and logos are
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reliable, however no responsibility is assumed by Analog Devices regarding the technical accuracy and topicality of the content provided in all Analog Devices’
Engineer-to-Engineer Notes.
a
-=5V
-=5V
18
ADSP-218x-/L/M/N DSP
ADSP-218x-/L/M/N DSP
V
V
DDINT
DDINT
GND
GND
18
17
17
L=3.3V
•
•
•
•
L=3.3V
M=2.5V
M=2.5V
C
C
N=1.8V
N=1.8V
4
4
C
C
FB
FB
••
••
••
C
C
IN
IN
GND
GND
12
12
CLKINXTAL
CLKINXTAL
C
C
IS
IS
••
C
C
R
R
FB
FB
••
••
1314
1314
••
••
••
C
C
FBS
FBS
••
C
C
OS
OS
OUT
OUT
CLKOUT
CLKOUT
V
V
••
CIS, C
CIS, C
ARE STRAY
ARE STRAY
CAPACITANCES
CAPACITANCES
FBS
FBS
, C
, C
OS
OS
••
•
Y
Y
1
C
C
1
1
1
•
C
C
2
2
L
L
1
1
C
C
3
3
16
16
15
15
•
DDEXT
DDEXT
GND
GND
•
17
17
•
•
COMPONENTS
COMPONENTS
ADDED
ADDED
FOR 3
FOR 3
OSCILLATOR
OSCILLATOR
C
C
5
5
RD
RD
OT
OT
-=5V
-=5V
L=3.3V
L=3.3V
M=2.5-3.3V
M=2.5-3.3V
N=1.8-3.3V
N=1.8-3.3V
Figure 1: Schematic of 3rd Overtone Crystal Oscillator
Note that the three capacitors, C
C
, must be ‘RF’ types with low loss dielectrics
3
, C2 and
1
at the frequencies being used. Examples of
capacitors with suitable dielectrics include silver
mica, polystyrene and ceramic NP0.
The inductor, L
, must also be chosen for
1
low RF losses (i.e. high ‘Q’). At these
frequencies and inductance values this usually
means an air core type, although there are some
inductors that use special formulations of iron
dust and/or ferrites that result in high Q. As a
guide, look for an inductor with a Q greater than
30, DC resistance less than 1.0Ω and a selfresonant frequency (SRF) greater than 120MHz.
The crystal’s load capacitance (C
) is
L
required to ensure the crystal operates at the
labeled frequency and will be specified by the
crystal manufacturer. This is usually a ‘standard’
value and 18pF is very common. It is up to the
engineer to choose the correct values for C
C
and L1 in conjunction with the amplifier and
3
, C2,
1
stray PCB capacitance, to provide the correct
load capacitance, C
. C1 and C2 will usually be
L
between 20pF and 70pF.
C
is only required for blocking DC
3
current that would otherwise load the output of
the oscillator. Its value is not critical and a value
of 1nF NP0 should be satisfactory.
with C
The inductor, L
and the stray output capacitance at a
2
, is chosen to resonate
1
frequency fR ≈ ⅔ of the 3rd OT frequency, fOT.
This provides the correct loading reactance for
the crystal and closed loop phase relationship to
start and maintain oscillation. In addition, the
parallel combination of L
an effective capacitance, C
frequency, f
, to correctly load the crystal.
OT
and C2 must provide
1
at the 3rdOT
2EFF
We have the following two equations
with two unknown values, L
2
f
OT
f
R
==
3
2
π
1
and C2 …
1
Equation 1
)(++
LCCC
12
OSOUT
×
XX
LC
12
f
,@
OT
+
X
C
EFF
XX
2
LC
12
1
Cf
EFFOT
2
Equation 2
==
2
π
EE-168: Using Third Overtone Crystals with the ADSP-218x DSP Page 2 of 11
a
where fR is the actual resonant frequency of L1
combined with the total output capacitance, C
C
and COS. Note that C2 is the actual
OUT
capacitor value used while C
capacitance at f
of C
and L1.
2
The reactance of C
due to the parallel combination
OT
3
is the effective
2EFF
is small enough to be
,
2
ignored. Similarly the contributions of the
feedback capacitances, C
and C
FB
, are very
FBS
small and can be ignored in determining the
required values of C
and L1.
2
With some simple arithmetic
manipulation we have the resulting design
equations for C
and L1 …
2
C++=
2
L++=
1
4
ω
where: ω
2
49
5
Equation 3
5
2
()
2
Equation 4
= 2πfOT
OT
CCC
OSOUTEFF
CCC
OSOUTEFFOT
()
Summarizing, the crystal manufacturer
will specify a total load capacitance for the
crystal. This is the TOTAL value of capacitance
that must appear across the two terminals of the
crystal for the operating frequency to be within
the specified tolerance of the value stamped on
the package. The total capacitance is usually
called the load capacitance, C
of the amplifier input capacitance, C
capacitance, C
and output capacitance, C
FB
, and will consist
L
, feedback
IN
.
OUT
Added to these is the PCB stray
capacitances, C
, C
IS
and COS. Finally we have
FBS
to add the external capacitors C1 and the parallel
combination of C
and L1.
2
Example: Determining External
Load Capacitors, C
Inductor L
Assume a manufacturer specifies a
37.5MHz 3
C
=18pF. For the ADSP-218xM/N oscillator
L
amplifier, typical values are C
7pF and C
capacitances, assume C
C
=1pF. These are all reasonable
FBS
approximations and, in practice, a couple of pF
either way will not make much difference.
To calculate the equivalent capacitance
across the crystal
output capacitances are effectively in series.
Therefore, the amplifier total capacitance,
C
:
AT
For the PCB total capacitance, C
Therefore, total Amplifier and PCB stray
capacitance, C
The total load capacitance is specified by
the crystal manufacturer. In this case, C
18pF. We have 6pF provided by the amplifier in
the DSP and stray PCB capacitance, as noted
above. Hence we have to add another 12pF in
parallel to make a total of 18pF. This
capacitance is provided by C
combination of C2 in parallel with L1.
1
rd
OT crystal with a load capacitance,
= 1pF. For the PCB stray
FB
=2pF, COS=3pF and
IS
, first note that the input and
C
= C
AT
+ CINC
FB
= [1+ 5×7/(5 + 7)]
≈ 4pF
C
PCBT
= C
+ CISCOS/(C
FBS
= [1 + 2×3/(2 + 3)]
≈ 2pF
:
ST
C
= CAT + C
ST
≈ 6pF
, C2 and
1
= 5pF, C
IN
/(C
OUT
IN
+ C
:
PCBT
+ COS)
IS
PCBT
and the
1
OUT
OUT
)
L
=
=
EE-168: Using Third Overtone Crystals with the ADSP-218x DSP Page 3 of 11
a
NOTE: It is most common to make C1
and C
the crystal, the resulting values for C
equal, and, since they are in series across
2
and C
1
2EFF
will each be 24pF, the series combination
making the 12pf required to make-up the
specified total load capacitance.
NOTE that this ‘sleight of hand’
introduction of capacitance C
in place of C2
2EFF
which is the effective capacitance of the parallel
combination of C2 and L1 required to make 24pF
at the 3rd OT frequency.
At this point we have determined the
value of C
- in this example,
1
C
= 24pF
1
From the design equations, 3 & 4, we can
determine the values of C
& L1,
2
= 662.2×10
-9
H
∴L1 = 662.2nH
Checking Calculated Values
To check the effective capacitance of the
C
//L1 combination at fOT, we can use the
2
expression;
1
+
ω
Lj
1
×
2
ω
Lj
1
1
2
×
L
1
C
2
which simplifies to;
EFF
EFF
ω
Cj
=
j
2
1
ω
ω
Cj
−=
CC
22
ω
()
C++=
2
C
2
2
= [9*24 + 4(7+3)]/5 = 51.2pF
49
5
∴C2 = 51.2pF
Also, knowing the required crystal
overtone frequency, ω
OT
2π×37.5MHz;
L++=
1
2
()
4
ω
5
2
L
= 5/[4(2π37.5×10E6)2(24+7+5)10E-12]
1
CCC
OSOUTEFF
= 2πfOT =
CCC
OSOUTEFFOT
Substituting values;
C
= 51.2pF – 1/(2π37.5E6)2×662.2E-9
2EFF
∴C
= 24pF 3
2EFF
Also, to confirm the frequency of
resonance, from equation 1;
f
= 1/[2π√{(51.2pF + 7pF + 5pF)662.2nH}]
r
∴fr = 25.0MHz = 2fOT/3 3
So all the calculations look good. Using
preferred values, we can complete our design as
shown in Figure 2. (See Appendix A for a
detailed component list)
EE-168: Using Third Overtone Crystals with the ADSP-218x DSP Page 4 of 11
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