AN2027 PSoC® 1 32.768-kHz External Crystal Oscillator.pdf

AN2027
PSoC® 1 - 32.768-kHz External Crystal Oscillator
Author: Jeff Dahlin
Associated Project: No
Associated Part Family: CY8C29x66, CY8C27x43,
CY8C24x23A, CY8C28xxx, CY8C2xx45
Related Application Notes: None
Many microcontroller applications require a timing source more accurate than the typical internal oscillator. An
external crystal can provide a solution. These crystals are used with an external crystal oscillator (ECO) to generate
®
clocks as accurate as ±50 parts per million. PSoC 1 can implement an ECO that uses a 32.768-kHz crystal.
Contents
Introduction
External Crystal Oscillator Theory .....................................1
Crystal Equivalent Circuit .............................................2
Crystal Selection ...............................................................2
Frequency of Oscillation ...............................................2
Load Capacitor Selection .............................................3
Drive Level ...................................................................4
Negative Resistance ....................................................5
PCB Layout Tips ...............................................................6
ECO Implementation Basics .............................................6
Providing a Local Bypass when Using PLL Lock Mode 7
Startup Requirements .......................................................8
Starting the ECO ..........................................................8
Starting the IMO PLL Mode ..........................................8
Recommendations .......................................................8
Using the ECO in Sleep ....................................................9
Sharing of ISSP and ECO Pins .........................................9
Dual Purpose ECO Pins ...............................................9
32-kHz ECO Using the CY3210 Kit ...................................9
Appendix A ...................................................................... 10
Observing ECO Operation.......................................... 10
Increasing the Drive Current....................................... 10
ECO_TR Register ...................................................... 10
Bit Description ............................................................ 10
Document History ............................................................ 12
Worldwide Sales and Design Support ............................. 13
PSoC 1 microcontroller’s external crystal oscillator (ECO)
can be used as a reference for timekeeping and other lowspeed (<32 kHz) operations. It can also act as the reference
for the phase-locked loop (PLL) mode of the internal main
oscillator (IMO). The PLL uses the 32.768-kHz input to
generate a more accurate 24-MHz clock signal. This is used
for operations that require an accurate high-speed clock
such as dual-tone multi-frequency (DTMF) signal generation,
serial communications, and RTC. Optimal performance from
the ECO for each of these functions requires different
external components and control register settings.
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External Crystal Oscillator Theory
The goal of clock generation is to synthesize a signal that
oscillates at a known frequency, duty cycle, and amplitude.
The clock signal is used to clock data into and out of digital
systems, and to govern the sampling of analog systems.
The ECO type used by PSoC 1 devices is a Pierce oscillator,
which is shown in Figure 1. The dotted box indicates that the
inverting amplifier is internal to the PSoC 1; all other parts
are external. The crystal input and output (XtalIn and
XtalOut) pins are also labeled in the diagram.
In this scheme, there are three discrete components, the
crystal (X1) and two load capacitors (CL1, CL2). These
components form a pi-network, which means that one
component is in series and the other two are connected to a
reference signal on either side.
Document No. 001-40399 Rev. *F
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PSoC® 1 - 32.768 kHz External Crystal Oscillator
Figure 1. Pierce Oscillator Topology
datasheet specifies the nominal frequency at which
crystal unit will oscillate. However, to successfully be
able to oscillate at the required frequency, sustaining
circuit must be carefully designed.
PSoC 1
Xi
CL1

Load capacitance – This is the capacitance that must
appear across the two terminals of the crystal. Any
deviation in the capacitance across the terminals will
cause a change in the oscillating frequency.

Drive Level – Drive level is used to express the
amount of power dissipated across the crystal unit. It
is expressed in microwatts (μW). A high drive level
may cause problems such as instability and aging. On
the other hand, a high drive level helps in better phase
noise performance. Thus, a compromise must be
established between the performance and aging.

Motional Resistance – Motional resistance or ESR
(effective series resistance) of the crystal is
responsible for the losses in the network. The
amplifier and external biasing network must
compensate for the losses across the ESR to maintain
a successful oscillation. This compensating of crystal
ESR via an amplifier and biasing network is referred
to as negative resistance of the oscillator circuit.
Xo
X1
CL2
Vref
The crystal or resonator (X1) in the pi-network is physically
designed to oscillate at the desired frequency. The
capacitors (CL1, CL2) in the pi-network “load” the crystal
or resonator to ensure proper oscillation. These capacitors
are referenced to VRef, which is VCC in PSoC 1 devices.
The inverting amplifier amplifies the output of the pinetwork and drives the input terminal with the logical
inverse. The pi-network provides 180 degrees of phase
shift from input to output at the resonant frequency. When
combined with the inverting amplifier, 360 degrees of
phase shift exist in the circuit, leading to oscillations at the
desired frequency.
These parameters are discussed in more detail in the
following sections.
Crystal Equivalent Circuit
Crystals can be modeled as a combination of passive
components. The equivalent model is shown in Figure 2.
C1 is known as the “motional capacitance” and L1 is
known as the “motional inductance”. C0 is known as the
“shunt capacitance”. Some or all of these characteristics
are specified by the crystal manufacturer.
Figure 2. Crystal Equivalent Circuit
X1
Frequency of Oscillation
The crystal oscillator works at two resonant frequencies,
series resonant (fs) formed by the series resonance of L1
and C1 and parallel resonant (fp) formed by the parallel
resonance of L1 and series combination of C1 and C0.
Parallel resonant frequency is also known as the
fundamental frequency of operation.
Figure 3. Resonator Reactance versus Frequency
=
R1
L1
C1
C0
Crystal Selection
Proper selection of crystal is important because along with
external components, internal parameters of the crystal
also play a crucial role in the signal generation of a
particular frequency. This section discusses the important
crystal parameters to be checked before using in a design.

Frequency of oscillation – A crystal is designed to
operate at a particular frequency. The manufacturer’s
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Document No. 001-40399 Rev. *F
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PSoC® 1 - 32.768 kHz External Crystal Oscillator
Figure 3 shows the reactance versus frequency curve of
the crystal. At frequencies far from fp, the crystal appears
capacitive; between fs and fp, it appears inductive. The
region between fs and fp is the usual operating range of
the crystal.
Crystal Selection
The crystals recommended for use with PSoC 1 are
parallel resonant, 32.768-kHz crystals.
Load Capacitor Selection
Crystal oscillator circuits must be loaded with the proper
capacitance to oscillate at the correct frequency. The pinetwork capacitors should be chosen based on the
chosen crystal’s rated load capacitance, as well as stray
capacitances from the PCB and PSoC pins. The total load
capacitance applied is equal to the series combination of
the two parallel combinations of the capacitances on each
of the crystal input and output pins.
When designing the ECO circuit, choose the value of two
discrete load capacitors, as shown in Figure 1. The circuit
actually contains additional parasitic capacitances, as
shown in Figure 4. Shown are the discrete load capacitors
(CL1 and CL2), along with PSoC pin capacitances (CP1
and CP2) and PCB trace capacitances (CB1 and CB2).
These parasitic capacitances will affect the applied load
capacitance and should be considered when a high
degree of accuracy is required. The total combination of
these capacitances should equal the rated load
capacitance of the crystal X1, which should be 12.5 pF.
Figure 4. ECO Circuit with Parasitic Capacitances
General Load Capacitance Criterion
CL 
Equation 1
1
1
1

CL1  CB1  CP1 CL 2  CB 2  CP 2
The package capacitances for the various PSoC MCU
packages are found in the Clocking section of the Device
Family Datasheets. The PCB trace capacitance depends
on PCB geometry. For example, a layout with 0.20-inch
long and 0.010-inch wide traces over a ground plane on a
4-layer 0.062-inch thick PCB, has a board parasitic
capacitance of 0.3 pF on each pin. This value may be
measured experimentally using an LCR meter, or
determined theoretically using the physical characteristics
of the PCB.
Balanced Load Capacitors
The most straightforward arrangement of discrete load
capacitors is to have the same value for both, a situation
that is described as “balanced”. Balanced configuration
provides an advantage of lower jitter when compared to
the unbalanced load capacitor configuration (discussed in
next section). If CL1 and CL2 are assumed to be equal,
the pin and trace capacitances are assumed to be the
same on input and output, and CL is assumed to be
12.5 pF, this relationship may be simplified, as shown in
the following equation.
Balanced Load Capacitor Criterion
Equation 2
CL1  CL2  25 pF  CP  CB
PSoC 1
Xi
disadvantages of different ratios are described in this
application note.
Table 1 shows standard balanced capacitor values that
are used with the various PSoC microcontroller packages,
assuming 0.3 pF board capacitance as in the previous
example.
Xo
Table 1. Example ECO Capacitor Values for Balanced
Feedback Configuration
X1
CP1 CB1 CL1
Package
CL2 CB2 CP2
Capacitor values may be determined using the formula
shown in General Load Capacitance Criterion
Equation 1. In this equation, CL1 and CL2 are the ECO
load capacitors shown in Figure 1, CP1 and CP2 are the
PSoC pin capacitances, and CB1 and CB2 are the printed
circuit board trace capacitances. When solving this
equation, CL, CB1, CB2, CP1, and CP2 will be known,
leaving one equation for two unknowns, CL1 and CL2. For
this reason, another equation must be generated,
describing the ratio between CL1 and CL2. This ratio will
differ between applications. The advantages and
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Typical CP
CL1
CL2
8-Pin DIP
0.9 pF
22 pF
22 pF
20-Pin DIP
2.0 pF
22 pF
22 pF
20-Pin SOIC
1.0 pF
22 pF
22 pF
20-Pin SSOP
0.5 pF
22 pF
22 pF
28-Pin DIP
2.0 pF
22 pF
22 pF
28-Pin SOIC
1.0 pF
22 pF
22 pF
28-Pin SSOP
0.5 pF
22 pF
22 pF
44-Pin TQFP
0.5 pF
22 pF
22 pF
48-Pin DIP
5.0 pF
20 pF
20 pF
48-Pin SSOP
0.6 pF
22 pF
22 pF
Document No. 001-40399 Rev. *F
3
PSoC® 1 - 32.768 kHz External Crystal Oscillator
Unbalanced Load Capacitors
By using an unbalanced pair of discrete load capacitors,
the amplitude of the input signal can be increased,
reducing the ECO’s noise susceptibility. In this case, the
series capacitance of the load capacitors still needs to be
the crystal’s rated load capacitance of 12.5 pF. An
unbalanced pair of capacitors causes an increase in the
operating current of the circuit, and is only recommended
for ECO designs with noise susceptibility problems.
For the unbalanced configuration, the total capacitance on
the XtalOut pin (Port 1, Pin 0) should be near 100 pF. The
following equation shows the total capacitance at the
XtalOut pin (CP1[0]) if a 100-pF discrete load capacitor is
used.
XtalOut (Port 1, Pin 0) Capacitance
Equation 3
CP1[0]  100 pF  CB2  CP2
CL1 
Equation 4
(CL2  CP 2  CB 2)  12.5 pF
 CP1  CB1
(CL2  CP 2  CB 2)  12.5 pF
Table 2 lists typical package capacitances and standard
capacitor values for CL1 and CL2 closest to the calculated
ideal values for various packages. Board parasitic
capacitance is assumed to be 0.3 pF for these
calculations.
Table 2. ECO Capacitor Values for Unbalanced Feedback
Package
Typical CP
CL1
Trim sensitivity is measured in PPM of added clock error
per pF of variation in total actual load capacitance. It can
be determined using crystal parameters described in the
Crystal Equivalent Circuit section. Trim sensitivity is a
function of the crystal’s rated load capacitance (CL), shunt
capacitance (C0), and motional capacitance (C1). The
function is shown in the following equation.
ECO Trim Sensitivity
The load capacitor at the XtalIn pin is chosen so that the
series capacitance at the crystal pins totals 12.5 pF.
Equation 4 shows the calculation for the ideal value of CL1
(the capacitor on P1[1]: XtalIn).
XtalIn (Port 1, Pin 1) Capacitance
Load Capacitance Trim Sensitivity
Variation of actual load capacitance has a tendency to
“pull” the resonant frequency of the ECO. This effect is
known as “trim sensitivity”. This effect can be both positive
and negative. On the positive side, the designer may tune
the resonant frequency of an oscillator by slightly
modifying capacitor values. However, on the negative
side, capacitance variation across parts and across
temperature can cause the generated frequency to differ
from the desired value.
CL2
8-Pin DIP
0.9 pF
12 pF
100 pF
20-Pin DIP
2.0 pF
12 pF
100 pF
20-Pin SOIC
1.0 pF
12 pF
100 pF
20-Pin SSOP
0.5 pF
12 pF
100 pF
28-Pin DIP
2.0 pF
12 pF
100 pF
28-Pin SOIC
1.0 pF
12 pF
100 pF
28-Pin SSOP
0.5 pF
12 pF
100 pF
44-Pin TQFP
0.5 pF
12 pF
100 pF
48-Pin DIP
5.0 pF
9 pF
100 pF
48-Pin SSOP
0.6 pF
12 pF
100 pF
Trim Sensitivit y  S 
Equation 5
C11,000,000
2
2 * C 0  CL 
Note This formula is a linearization of what is actually a
second order function. For more details, ask your crystal
vendor.
For example, here we calculate trim sensitivity for an
Abracon AB38T-32.768-kHz crystal. This 32.768-kHz
crystal has a typical C1 of 0.0035 pF, typical C0 of 1.6 pF,
and CL of 12.5 pF. Thus, the trim sensitivity is determined
as shown in Equation 6. This calculation shows that for
1 pF in error in the actual load capacitance, the frequency
will shift by 8.8 PPM or 0.29 Hz.
Note 1 pF in discrete capacitor error will cause less than
1 pF of total actual load capacitance error, because of the
relationship shown in Equation 1.
Trim Sensitivity Calculation Example
S
Equation 6
C11,000,000 0.0035 1,000,000
PPM

 8.8
2
2
pF
2 * C 0  CL 
2 * 1.6  12.5
Trim sensitivity implies requirements for load capacitor
values and temperature coefficients. It should be
considered along with resonator frequency accuracy and
system performance requirements to determine what load
capacitors to use.
Drive Level
Drive level of a crystal indicates the amount of current
flowing through its electrodes. It is expressed as the power
dissipation across the crystal unit. Drive level has a strong
effect on the frequency of oscillation, and can adversely
affect the crystal performance as well. It is important to
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Document No. 001-40399 Rev. *F
4
PSoC® 1 - 32.768 kHz External Crystal Oscillator
understand the advantages and limitations of having
higher drive levels.
Advantages:

Higher drive level helps in meeting the startup
requirement of higher gain to compensate for the drop
across the ESR of the crystal.

Higher drive level provides better phase-noise
performance (deviation in phase causes the frequency
to change in order to maintain the 2-nπ phase
condition).
Negative resistance model is widely used for the analysis
of oscillation circuitry because it accurately determines
whether the system provides sufficient gain to build the
oscillation. Figure 5 explains the negative resistance
model.
Figure 5. Negative Resistance Model
I
Limitations:
As the drive level increases, the amplitude of crystal
oscillations also increase. It may cause excessive
aging and in some cases the crystal may also break.

Increasing drive level can also cause shift in the
oscillation frequency because of the temperature
increase due to the dissipation across the crystal.
Active Branch

R1
XOSC
X1
Motional Branch
-RNEG
To ensure that drive level of the crystal unit is kept in
control, the PSoC 1 device family has an inbuilt Automatic
Gain Control (AGC), which reduces the gain of the
amplifier if it crosses a particular threshold. The AGC is
always active and cannot be turned off. This helps to
reduce the drive level and has better stability.
Drive level can be expressed by Equation 7.
Drive Level
Equation 7
DL  IL _ RMS2 * R1
Similar to the Barkhausen criteria or oscillation, the
negative resistance model is given by Equation 8 and
Equation 9.
R NEG  R1
Equation 8
where, IL_RMS is the RMS current through the crystal, and
R1 is the motional resistance of the crystal.
XOSC  X1
Equation 9
Drive level is measured using a current probe, which
measures the current entering or exiting the resonator.
The ECO should be tested in the intended final
configuration, without any resistance used for testing –R.
The current measurement should be taken after ECO
startup is complete and the automatic gain control has had
time to stabilize at the steady state drive level of the
circuit. The RMS current measurement may be used in
conjunction with Equation 7 to calculate drive level.
In the steady state, the oscillator must provide sufficient
negative resistance to compensate for the losses in the
resistance of the crystal. The reactive component of the
crystal must cancel the reactive component of the
oscillator; this determines the frequency of oscillation.
Equation 8 and Equation 9 are valid only for the steady
state. However when the oscillations build up, negative
resistance must be higher to ensure that more energy is
delivered to the crystal motional arm to build up the
oscillations.
C r ys t a l S e l e c t i o n
Drive level of a crystal is mentioned in the manufacturer’s
datasheet. It is strongly recommended to not drive the
crystal at a rating higher than the one mentioned in the
crystal’s datasheet.
Table 3 provides some generic guidelines for the –R to
ESR ratio for startup.
Table 3. –R to ESR Ratio Guidelines
Ratio (–R : ESR)
Negative Resistance
Negative resistance is not a physical parameter but is
named after the change in the I-V characteristics of a
tunnel diode when operated in a particular region. In
tunnel diode, with the increase in voltage, it exhibits a dip
in current. This effect is known as negative resistance.
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Mode of Operation
Ratio < 2:1
Unsafe
2:1 < Ratio < 3:1
Suitable
3:1 < Ratio < 5:1
Safe
5:1 < Ratio
Very safe
Document No. 001-40399 Rev. *F
5
PSoC® 1 - 32.768 kHz External Crystal Oscillator
Negative resistance of an oscillator circuit is governed by
a number of factors, which include amplifier gain or drive
level, external components, and shunt capacitance of the
crystal.
C r ys t a l S e l e c t i o n
Lower the shunt capacitance, higher will be the –R and
lower the ESR, lower will be the requirement for –R
It is important to consider that SMD crystals have lower
shunt capacitance, but their ESR is generally on a higher
side (typ. 60 kΩ). If higher ESR crystals are used with
0
PSoC 1 or device is intended to operate at less than 0 C,
then it is recommended to increase the amplitude level
(see Increasing the Drive Current section) to meet the –R
to ESR ratio requirement.
The ECO drive circuitry must be electrically connected to a
32,768 Hz crystal through the XtalIn and XtalOut pins of
the PSoC MCU.
Note 32,768 Hz is used because it allows the power of
two integer division to a 1-Hz clock signal, because 2^15 =
32,768.
The XtalIn and XtalOut pins must have their drive modes
set to HI-Z (highlighted in Figure 7) for the ECO to work
properly. If the pin drive modes are not set to HI-Z, the
drive circuitry will free-run at an incorrect frequency.
Figure 7. XtalIn and XtalOut Pin Drive Settings for ECO
Operation
PCB Layout Tips
The ECO operates as a low-power oscillator. To
accomplish this, it is designed as low-amplitude, highimpedance analog circuit. It must be treated as such
during component placement and circuit layout. Layout is
critical to performance. Also, note that the presence of
contaminants on the PCB impacts the performance of the
oscillator.
The crystal and the load capacitors must be placed close
to the pins of the microcontroller. They must be placed
over a common-ground plane. High-speed digital signals
(signals with short rise and fall times) should not be routed
close to the ECO circuit. Also, digital signals should not be
routed near the ECO external components. When
possible, the pins immediately adjacent to the ECO pins
must be left unconnected or they must be used for lowerspeed signals. Low-speed signals may be driven with the
“strong slow” setting.
The pins are automatically set to High Z if the “Select”
parameters are set to XtalOut and XtalIn in the Pin
Description table. The correct configuration of P1[0] and
P1[1] is confirmed by running the Design Rule Checker in
PSoC Designer (Tools > Design Rule Checker); you can
see the results in the output window.
ECO Implementation Basics
Figure 8. Design Rule Checker Output
Figure 8 shows the output of the DRC when P1[0] and
P1[1] are not correctly configured.
The PSoC microcontroller’s 32.768-kHz clock uses either
the low-accuracy ILO or the higher accuracy ECO for
reference. The 32-kHz Select bit of the Oscillator Control
Register 0 (OSC_CR0) determines which source is used.
The easiest way to set this bit is to set the 32K_Select
parameter in the Global Resources table of PSoC
Designer™ to ‘External’ (highlighted in Figure 6).
Figure 6. 32K_Select Setting for ECO Operation
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Document No. 001-40399 Rev. *F
6
PSoC® 1 - 32.768 kHz External Crystal Oscillator
Figure 10. PLL_Mode Setting for IMO Operation
ECO and PLL Mode
The IMO maybe be sourced with a signal from the PLL,
using the ECO as a reference. This results in an IMO with
a more accurate frequency and less voltage and
temperature drift than can be accomplished with the IMO
alone. Normally, the IMO operates with 2.5 percent
accuracy over the full temperature and voltage range.
When using the PLL, the IMO can be as accurate as the
ECO itself, less than ±100 PPM of error, depending on the
ECO configuration.
When configuring the IMO in PLL mode, a number of
changes must be made. The design must use an
unbalanced load capacitor configuration and include a
local bypass capacitor. Also, an increased drive current
must be used. The unbalanced feedback configuration has
already been discussed, and increased drive current is
described later in this document.
The use of unbalanced load capacitors boosts the
amplitude of the signal at XtalIn (P1[1]). See Figure 9 for a
waveform at P1[1], captured with the aid of the circuit
shown in Figure 15. See Observing ECO Operation to
understand how to view ECO signal on an oscilloscope.
The amplitude at XtalIn is now approximately 600 mVp-p.
Figure 9. ECO Waveform with Unbalanced Capacitors
In general, a PLL requires a low jitter reference to remain
stable. Because the PSoC microcontroller’s ECO uses a
low-amplitude signal, the presence of noise causes the
apparent position of the clock edges to jitter from cycle to
cycle. The base frequency of the ECO remains accurate
but the jitter can cause the IMO to be unstable. The
purpose of the unbalanced load capacitors is to reduce the
jitter caused by noise on the 32-kHz waveform.
When using the PLL mode of the IMO, PCB layout is the
most critical factor in minimizing jitter on the ECO. By
carefully designing the PCB, the amount of noise present
in the ECO circuit can be minimized. See PCB Layout Tips
for more details.
Other required modifications to increase the stability of the
ECO are providing a local VCC bypass and increasing the
ECO drive current.
Providing a Local Bypass when Using PLL
Lock Mode
When using the PLL configuration of the IMO, additional
filtering of the VCC power is required. For this purpose, a
local VCC bypass capacitor is added near the XtalIn pin
(Port 1, Pin 3). To do this, configure the pin’s drive mode
to Resistive Pull Down and write a ‘1’ to the Data Register
(PRT1DR). Connect the pin to VCC and connect a 0.1-µF
capacitor between the pin and VSS (see Figure 11). This
connects the internal power bus to VCC through the pin
pull-up FET; providing a local low-impedance connection
to VCC.
Figure 11. PLL Mode Electrical Configuration
The PLL Mode bit of the OSC_CR0 register enables the
PLL mode of the IMO. The easiest way to set this bit is to
set the PLL_Mode parameter to ‘Ext Lock’ in the Global
Resources window of PSoC Designer (highlighted in
Figure 10).
Vcc
CBypass
P1[1]
Internal Vcc
"1"
P1[0]
Vcc
CL2
X1
A drive mode of Pull Down is recommended so that if a ‘0’
is accidentally written to P1[3] it results in a 5.6-kΩ
resistance between VDD and VSS, instead of a short
between VDD and VSS.
CL1
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Document No. 001-40399 Rev. *F
7
PSoC® 1 - 32.768 kHz External Crystal Oscillator
Startup Requirements
Both the ECO and IMO experience periods of instability
when they are first started. Therefore, the ECO output is
not used as a source for the internal 32-K clock or as a
reference for the PLL mode of the IMO until it has had
time to stabilize. The IMO experiences a frequency
overshoot when the PLL is first enabled. As a result, the
CPU clock speed must be lowered when the IMO is
initially switched to PLL mode to prevent the CPU clock
from exceeding its operational limit.
the ECO, but does not wait for it to stabilize and does not
set the PLL_Lock bit. If this is done, you must provide
code elsewhere that enables the ECO through the same
process as the original startup sequence. However, for
this to work, the PLL_Mode must be disabled in the Global
Resources window so that it is not enabled by boot.asm
before the ECO is enabled by the user’s code. If the PLL
is used in the application, it must also be enabled by the
user’s code after the ECO is enabled correctly.
Starting the IMO PLL Mode
These circumstances require the ECO and IMO PLL mode
to follow a specific startup sequence. The boot.asm meets
this requirement if the appropriate settings (32KSelect =
External and PLL_Mode = Ext Lock) are selected in the
Global Resources grid in the Device Editor of
PSoC Designer.
The IMO cannot be phase-locked to the ECO until the
ECO is stable—this takes approximately one second.
Also, the CPU clock frequency cannot exceed 3 MHz
when the PLL mode is first set. Both of these restrictions
are in place to prevent the CPU clock frequency from
temporarily exceeding 12 MHz for 3 V operation (or
24 MHz for 5 V operation).
Starting the ECO
As mentioned earlier, boot.asm holds off entry to main()
until all of the clocks are stable when using the ECO.
When the PLL mode is used, the following delays are also
present in boot.asm:
When the ECO is first enabled, its output is not connected
to the 32-K clock tree within the PSoC microcontroller.
Instead, the 32-K clock continues to be driven by the ILO
until the ECO has had time to stabilize. This time is
approximately 1 second. The boot.asm configures the
sleep timer for 1 second, and then waits until the sleep
timer reaches terminal count. With this mechanism, the
sleep timer is used to delay connecting to the ECO until its
output has stabilized.


The following steps are followed by boot.asm when
starting the ECO:
1.
The sleep timer is set to one second and cleared. The
sleep timer interrupt need not be enabled.
2.
ECO is enabled; set the 32-K Select bit of OSC_CR0
to ‘1’.
3.
When the sleep timer reaches terminal count (one
second later), the ECO is automatically selected as
the source for the 32-K clock tree and can now be
used as a clock source for event timing.
The boot.asm holds off entry to main() until all the clocks
are stable. This means that calling main is delayed by
about one second when using the ECO.
Note The sleep timer uses the ILO, which is –50% to
+100% accurate, so this “1 second” sleep time can vary
from 0.5 to 2 seconds.
If some tasks must be accomplished before the onesecond period expires, add the initialization code to
boot.asm (remember that the edits must be made to the
template file: boot.tpl). You can also choose to write your
own clock initialization code as long as the rules in this
section are upheld.
The boot.asm contains a flag, WAIT_FOR_32K, which
forces the program to wait for the clocks to stabilize before
calling main. If you change this flag to ‘0’, boot.asm starts
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A one-second delay is added whenever the ECO is
enabled to wait for the ECO to become stable.
Following the one-second delay, the CPU speed is
set to 3 MHz, PLL is enabled, and a delay of 16 ms is
introduced. After the 16-ms delay, the CPU speed is
set to 12 MHz and the rest of the initialization code
continues.
Note The CPU speed is set to the desired speed as
configured in the Global Resources at the end of
boot.asm.
Recommendations
Under normal conditions, the recommended setting for the
External Crystal Oscillator Trim (ECO_TR) register is 7Ah.
The ECO_TR register sets the adjustment for the 32.768kHz ECO. This is the lowest amplitude setting with output
buffer B bias control enabled. For higher gain settings,
amplitude of the ECO_TR register can be changed. Make
sure that the drive level is below the maximum limit
specified in the crystal datasheet. See Table 4 for
reference.
Notes
1.
Setting the 32K_Select Global Resource to ‘Internal’
and PLL_Mode Global Resource to ‘External Lock’ is
an invalid configuration. There is no connection from
the ILO to the IMO (see the Clock Tree diagram in the
CY8C27x43 Family Datasheet). The requirement is
evaluated by the Design Rule Checker provided in
PSoC Designer (Tools > Design Rule Checker).
2.
The XtalIn and XtalOut pins are also used for
in-system serial programming (ISSP). The pins can
be configured to function for both operations in the
Document No. 001-40399 Rev. *F
8
PSoC® 1 - 32.768 kHz External Crystal Oscillator
3.
same design. For more information on in-system
programming, see PSoC 1 – ISSP Programming
Specifications.
portion of the schematic is shown in Figure 12, and a
picture of the related portion of the PCB configured for
ECO use is shown in Figure 13
For the CY8C27x43 Rev. A chip, bits 2 and 3 of
CPU_SCR1 register cannot be used.
To install and use a 32.768 kHz ECO with the CY3210EVAL1 kit, perform the following steps:
Using the ECO in Sleep
The 32-kHz ECO may be used as a clock source for digital
blocks during sleep, but care must be taken to
desynchronize the clock inputs from the IMO, because it
will be turned off. If any clock is synchronized to a static
signal, all clock edges will be masked.
1.
Remove resistors R8 and R9.
2.
Install a 0805 12 pF capacitor as C10.
3.
Install a 0805 100 pF capacitor as C9.
4.
Install a can-style 32.768-kHz, 12.5-pF crystal as Y1
(such as Abracon AB38T – 32.768KHz).
Figure 12. ECO Portion of CY3210-EVAL1 Kit Schematic
Digital block input clock resynchronization is controlled
using the AUXCLOCK[7:6] bits in the DxBxxOU registers.
A value of 0x00 in the AUXCLOCK bits will select the
unsynchronized clock input. Clock synchronization is
described in depth in the PSoC 1 TRM sections “Input
Data Synchronization” for both analog and digital blocks.
Sharing of ISSP and ECO Pins
Dual Purpose ECO Pins
In PSoC 1 family, Xin and Xout pins of ECO are on P1.1
and P1.0, which are also the dedicated pins for ISSP
programming. This dual functionality of ISSP/ECO pins
does not add any constraint on ISSP lines because the
capacitor required on Xin and Xout lines are in the order of
10 to 100 pf, which does not impose any problem for ISSP
programming protocol. But capacitance added to Xin and
Xout because of ISSP traces and connector may cause a
shift in crystal's oscillating frequency (discussed in section
Load Capacitor Selection). For precise frequency
generation following guidelines should be followed:

Keep ISSP traces as small as possible to minimize
the additional capacitance.

Compute the value of C1 and C2 by considering the
capacitance of ISSP traces into account.
Figure 13. CY3210-EVAL1 ECO Components
OR

For production boards, add a 0-Ω resistor in between
ISSP header and pins. Remove 0-Ω resistors to
remove the capacitance during operation.
32-kHz ECO Using the CY3210 Kit
The CY3210-EVAL1 kit has traces and footprints to allow
the installation of a 32.768-kHz crystal and pi-network
capacitors. The crystal network is connected to pins P1[0]
and P1[1]. These pins are also connected to a header for
use as standard GPIOs. This connection is made through
0-Ω resistors R8 and R9, so that the parasitic capacitance
of these traces may be removed from the oscillator. This
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Note The label for component Y1 is beneath the body of
the crystal can, and is thus not visible in this picture.
Document No. 001-40399 Rev. *F
9
PSoC® 1 - 32.768-kHz External Crystal Oscillator
Appendix A
Figure 16. ECO Electrical Connections
Observing ECO Operation
Because the ECO circuit is high-impedance and lowamplitude, a standard oscilloscope probe cannot be used to
view the signal. The load of a standard oscilloscope probe
distorts the waveform and impacts performance. One option
is to use a unity gain opamp to buffer the signal so that it is
viewed with an oscilloscope. Figure 14 shows the ECO
waveform at the XtalIn pin (P1[1]) captured with the aid of
the circuit shown in Figure 9.
Figure 14. ECO Waveform
Vdd
P1[1]
PSoC 1
CL1
X1
P1[0]
Vdd
CL2
For standard ECO operation (when not used as a reference
for the IMO PLL), the configurations described in the Device
Family Datasheets should be used. This includes a
32.768 kHz, 12.5 pF, 1 µW or less watch crystal, and
temperature stable (NPO) ceramic capacitors.
Increasing the Drive Current
To increase the drive current of the ECO network, update
the ECO_TR register. This register controls the amplitude
level of the amplifier used available inside PSoC 1.
ECO_TR Register
When using the ECO, there are a few components that must
be set by the trim register for satisfactory operation. They
include Comparator or Output Buffer A and B and the
Amplitude Control. Output Buffer A is an improvement from
an older design while Output Buffer B is a new addition. The
ECO_TR register is write only, which means that bitwise
logical operations cannot be used to change specific bits.
This register is shown in Table 4.
Figure 15. Unity Gain Buffer
Connect to
P1[1]
Vdd
+
National
Semiconductor
LMC6482A
Connect to
Oscilloscope
Vss
The analog signal has a DC offset of approximately 4 V and
peak-to-peak amplitude of approximately 400 mV.
Figure 16 shows the external circuit that is used for the ECO.
Note that the load capacitors are connected to VCC. This is
the optimal configuration because the ECO driver is
referenced to VCC. If the capacitors are incorrectly
referenced to VSS, the ECO will operate at the correct
frequency, but is slightly more susceptible to power supply
noise.
Bit Description
Output Buffer ‘A’ Bias Control [0]
This bit is used to set the startup (unregulated) bias current
of the crystal oscillator output buffer A. In normal operation,
this bias level exceeds what is required for stable oscillation
and as a result, the amplitude of the signal on the crystal
increases. The signal then approaches the level set by the
amplitude control bits and the bias level is reduced by the
amplitude control loop until stable oscillation is maintained at
the defined level.
0 = minimum bias
1 = maximum bias
Output Buffer B Bias Control [1]
This bit is used to set the bias reference level for the crystal
oscillator output buffer B. Because output buffer B uses a
fixed bias level, this operates at a fixed level independent of
the oscillator amplitude settings.
0 = minimum bias
1 = maximum bias
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Document No. 001-40399 Rev. *F
10
PSoC® 1 - 32.768-kHz External Crystal Oscillator
Amplitude Control [3:2]
These bits are used to control the amplitude of the crystal
oscillator. The settings are:
01 = Highest
00 = Medium High
1 = enables operation for buffer B and bias generator
O u t p u t B u f f e r B H ys t e r e s i s E n a b l e [ 5 ]
This bit provides approximately 30 mV of hysteresis to the
output buffer. However, the value of bit 5 elicits no effect if
output buffer B is not enabled by bit 4.
0 = Disables Hysteresis
11 = Medium Low
1 = Enables Hysteresis
10 = Lowest
Output Buffer B Enable [4]
This bit is used to enable the extra output buffer B. This
buffer operates at a fixed bias level, which is controlled by
the bias control bit 1. That also means that bit 1 elicits no
effect if bit 4 does not enable buffer B.
R e s e r ve d [ 6 :7 ]
These bits are unused by this operation, but are assigned to
functions elsewhere in the IC.
0 = enables operation only for buffer A
Table 4. ECO_TR Register Description
Bit 7
Bit 6
Reserved
Reserved
Bit 5
Bit 4
Output Buffer
Output Buffer
B Hysteresis
B Enable
Output Buffer B Control
Bit 3
MSB
Bit 2
LSB
Amplitude Control
Bit 1
Bit 0
Output Buffer
Output Buffer
B Bias Control
A Bias Control
Bias Control
Table 5. Amplitude Setting
Amplitude Setting
ECO_TR
Highest
0x77
Medium High
0x73
Medium Low
0x7F
Lowest
0x7B
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Document No. 001-40399 Rev. *F
11
PSoC® 1 - 32.768-kHz External Crystal Oscillator
Document History
®
Document Title: PSoC 1 - 32.768-kHz External Crystal Oscillator - AN2027
Document Number: 001-40399
Revision
ECN
Orig. of
Change
Submission
Date
Description of Change
**
1532004
EDT
11/13/2007
Submitted to ECN system
*A
2551067
MAXK/JVY
08/11/2008
Rolled in changes from multiple revisions that were never formalized. Updated for
more recent devices and programming software.
*B
3157509
MAXK
01/30/2011
Added CY3210 kit details. Added operation in sleep. Updated title and abstract.
*C
3266143
MAXK
05/25/2011
Added CY8C28xxx, CY8C2xx45 to Associated Part Family.
*D
3478292
MAXK
12/29/2011
Added information on ECO theory, equivalent model, and trim sensitivity
Updated load capacitor nomenclature to CL1 and CL2
Improved diagram clarity
Updated template
*E
3714751
PMAD
08/16/2012
Added selection information for drive level and negative resistance.
Added advantages of balanced capacitor configuration.
Added Appendix A and Sharing of ISSP and ECO Pins.
Updated template.
*F
4422007
www.cypress.com
PMAD
06/27/2014
Updated template. Sunset Review.
Document No. 001-40399 Rev. *F
12
PSoC® 1 - 32.768-kHz External Crystal Oscillator
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Document No. 001-40399 Rev. *F
13