Technical Note 31 - Statek Corporation

TECHNICAL NOTE 31
Practical Analysis of the Pierce Oscillator
Introduction
To achieve optimum performance from a
Pierce crystal oscillator, e.g. good frequency
stability and low long term aging, the crystal
parameters, crystal drive current, and
oscillator gain requirements must be
carefully considered. Over many years of
experience, it has been found that
excessive crystal drive current is one of the
main causes of oscillator malfunction.
Overdriving the crystal causes frequency
instability over time, and for tuning-fork
crystals
the
excessive
motional
displacement can break the crystal tines.
(a) The loop gain must be greater than
unity.
(b) The phase shift around the loop must
be an integer multiple of 2π.
The CMOS amplifier provides the
amplification while the two capacitors CD
and CG, the resistor RA, and the crystal work
as the feedback network. The resistor RA
stabilizes the output voltage of the amplifier
and is used to reduce the crystal drive level.
This technical note describes a practical
approach to measuring the key parameters
of a Pierce oscillator. This allows the
designer to check the oscillator design
against the actual oscillator performance
and ensure that the oscillator design rules
are met.
(For analysis, see Statek
Technical Note 30.) This note covers the
following topics:
1. A practical procedure for determining
the crystal drive current.
2. A practical procedure for measuring the
amplifier’s transconductance gm and
output resistance RO.
3. A practical procedure for determining
the total load capacitance CL of the
Pierce oscillator circuit.
Basic Crystal Oscillator
The basic quartz crystal CMOS Pierce
oscillator circuit configuration is shown in
Figure 1.
The crystal oscillator circuit
consists of an amplifying section and a
feedback network. For oscillation to occur,
the Barkhausen criteria must be met:
Figure 1: Basic Pierce Oscillator Circuit
The crystal drive current is given by the
equation



ib = 




2
 X e   Re 

1 +
 + 
 X 0′   X 0′ 
2
2


′  

 Re + RA 1 − X e   +  X e′ + RA Re 
 X ′  

X D 
0 



2



V ,




where
X 0′ =
1
1
.
=
ωC0′ ω (C0 + Cs )
The gain equation is
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Page 2 of 4
[
gm > 4π f CG (CD + Cd) Re +
+
CG
( )
RA
CD 1+ R +Cd
O
(
2 2
4π f CdCDRA +
1
RO
(
Cd +
)(
1+
Re
C
RO d
) ]
RA
)
2 2
RA + Re
-4π f CdCDRA Re
RO
The operating frequency is given by
scope probe to avoid changing the DC
bias voltage.
6. Calculate the peak-to-peak currents:
(IG)p-p = (VG)p-p/XG and (ID)p-p = (VD)p-p/XD.
7. Calculate the RMS currents: (ID)RMS =
(ID)p-p/ 2 2 and (IG)RMS = (IG)p-p/ 2 2 .
( )
( )


C1
 ,
f = fs 1 +
 2(C0 + CL ) 
8. The AC current through the crystal will
be between (IG)RMS and (ID)RMS, being
closer to (IG)RMS.
where CL is the load capacitance of
oscillation. The equations for the oscillation
frequency, gain and crystal drive are
derived using a closed loop and phase
diagram analysis of a CMOS quartz crystal
oscillator. For more details see Statek’s
Technical Note 30.
9. The measured current should not
exceed the maximum recommended
value
Measuring the Crystal Drive Level
Measuring the Transconductance
and Output Impedance of the
Amplifier
One of the most important parameters for a
good oscillator design is the crystal drive
current. With increasing demand for ultra
miniature quartz crystal resonators, the
crystal parameters and the oscillator
components must be carefully considered.
The maximum recommended crystal drive
level should not be exceeded.
IRMS ≤
(maximum allowed power ) .
R1
For the oscillator to start up, the
transconductance of the amplifier must be
greater than the value given by the gain
equation, and as a general rule it is best
that it at least 2-3 times this minimum.
The main factors affecting the drive level
are the supply voltage (VDD), R1, RA, CD, CG,
and the stray capacitance, Cs.
Measurement Procedure
1. Measure CG: Remove the crystal and
neutralize node (d). With no power
applied,
measure
CG
using
a
capacitance meter.
2. Measure CD: Remove the crystal and
disconnect RA. With no power applied,
measure CD and Cd using a capacitance
meter.
3. Calculate the impedances XG =1/(ωCG),
XD = 1/(ωCD), and Xd = 1/(ωCd).
4. Mount the crystal, reconnect RA and turn
on the operating supply voltage.
5. Using a scope probe with no more
than 2 pF capacitance, measure the
peak-to-peak voltages across CG and
CD. Note: AC-couple the signal to the
Figure 2: Measuring the Transconductance
and Output Impedance of the Amplifier
Measurement Procedure
1. Apply a sinusoidal voltage VI to the input
of the amplifier, coupled through a 1 µF
capacitor (with the voltage sufficiently
low so that the output does not
saturate). (See Figure 2.)
2. Measure the output voltage VO through a
1 µF capacitor.
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3. Measure the output voltage with various
load resistances to ground.
For example consider the sequence of
measurements in Table 1.
Table 1: Measuring RO
VO [V]
VI [V] RL [kΩ]
0.0168
OPEN
1.068
0.0168
30
0.636
0.0168
18
0.520
0.0168
15
0.464
The output resistance RO of the amplifier is
approximately equal to that load resistance
RL such that the output voltage VO is one
half of the output voltage when the load
resistance is infinite (open). In the above
example, at a load resistance RL of 18 kΩ,
the output voltage VO is approximately equal
to one-half of VO when RL is an open circuit.
Therefore, RO is equal to approximately
18 kΩ.
The amplifier’s transconductance gm is the
equal to the voltage gain divided by RO.
g m = (VO / VI ) / RO
= (1.068 / 0.0168) /(18 kΩ)
= 3.53 mS.
Table 3: Crystal Parameters
2. Measure stray capacitance Cs across
the crystal: Remove the crystal,
neutralize the positive (Vdd) and ground,
then measure the capacitance across
the crystal termination.
Table 2: Oscillator Parameters
Gate capacitance
Drain capacitance
Stray capacitance
Amp. Output capacitance
Amp. Output resistance
Limiting resistance
Symbol
CG
CD
Cs
Cd
RO
RA
Value
7.4
5.4
1.4
7.0
70
30
Unit
pF
pF
pF
pF
kΩ
kΩ
Value
1.0
3.0
1.2
Unit
MHz
KΩ
pF
Using the gain equation, we find for the
oscillator and crystal described in Tables 2
and 3
g m ≥ 0.119 mS .
The
ratio
of
the
amplifier’s
transconductance
to
the
minimum
transconductance required for oscillation is
(3.53/0.119) = 29.7. Therefore, this circuit
meets both the required minimum
transconductance and the 2-3 times the
minimum rule.
Measuring the Load Capacitance of
the Oscillator Circuit
Properly specifying the load capacitance of
the oscillator circuit allows the crystal
manufacturer to tune the crystal frequency
to the operating frequency of the oscillator.
Given a crystal of known fs, C1, and C0,
operating at a frequency f in a circuit, the
load capacitance of the circuit is found from
the frequency equation
The required minimum transconductance of
the oscillator is calculated as follows:
1. Measure CG and CD, as described
above.
Symbol
fs
R1
C0
Frequency
Motional resistance
Shunt capacitance
CL =
C1  fs 

 − C0 .
2  f − fs 
Measurement Procedure
1. Measure the crystal parameters C1, C0,
and fs with the use of a CI meter or an
impedance analyzer.
2. Install the measured crystal in the
oscillator circuit and measure the
oscillation frequency f.
3. Then calculate the load capacitance CL.
For example with
fs
C1
C0
f
=
=
=
=
32.7644 kHz
2.3 fF
1.5 pF
32.768 kHz
=
9.0 pF.
we find
CL
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The calculated load capacitance includes
the stray capacitance across the crystal
(Cs).
Glossary
Table 4: Glossary of Symbols
L1
C1
C0
R1
RA
fs
f
VI
VO
CL
Cs
CD
CG
ib
gm
RO
Cd
Crystal Motional Inductance
Crystal Motional Capacitance
Crystal Shunt Capacitance
Crystal Motional Resistance
Limiting Resistance
Series Resonant Frequency of
the Crystal
Operating Frequency
Input Voltage
Output Voltage
Total Load Capacitance of the
Oscillator
Total Stray Capacitance Across
the Crystal
Drain Capacitance
Gate Capacitance
Crystal Drive Current
Transconductance
Amplifier Output Resistance
Amplifier Output Capacitance
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STATEK Corporation, 512 N. Main St., Orange, CA 92868 714-639-7810 FAX: 714-997-1256 www.statek.com