ATMEL U4223B-MFS

U4223B
Time-Code Receiver with A/D Converter
Description
The U4223B is a bipolar integrated straight-through receiver circuit in the frequency range of 40 kHz to 80 kHz.
The device is designed for radio-controlled clock applications.
Features
Very low power consumption
Only a few external components necessary
Very high sensitivity
4-bit digital output
High selectivity by using two crystal filters
AGC hold mode
Power-down mode available
Block Diagram
PON
CLK D3
17
12
16
VCC 1
D1
18
D0
19
20
11
ADC
Power supply
GND
D2
Decoder
10
3
9
FLB
FLA
DEC
Impulse
circuit
IN
AGC
amplifier
2
13
Rectifier &
integrator
15
7
8
SB Q1A Q1B Q2A Q2B
REC
INT
4
5
6
14
SL
Figure 1. Block diagram
Ordering and Package Information
Extended Type Number
U4223B-MFS
U4223B-MFSG3
T4223B-MF
T4223B-MC
Rev. A7, 06-Mar-01
Package
SSO20 plastic
SSO20 plastic
No
No
Remarks
Taping according to IEC-286-3
Die on foil
Die on carrier
1 (18)
U4223B
Pin Description
VCC
1
IN
2
20
D0 (LSB)
19
D1
GND
3
18
D2
SB
4
17
D3 (MSB)
Q1A
5
16
PON
15
Q2B
14
Q2A
U4223B
Q1B
REC
INT
DEC
FLA
6
7
13
8
12
9
11
10
SL
CLK
FLB
Pin
Symbol
Function
1
VCC
2
IN
3
GND
4
SB
5
Q1A
Crystal filter 1
6
Q1B
Crystal filter 1
7
REC
Rectifier output
8
INT
Integrator output
9
DEC
Decoder input
10
FLA
Lowpass filter
11
FLB
Lowpass filter
12
CLK
Clock input for ADC
13
SL
14
Q2A
Crystal filter 2
15
Q2B
Crystal filter 2
16
PON
Power ON/OFF control
17
D3
Data out MSB
18
D2
Data out
19
D1
Data out
20
D0
Data out LSB
Supply voltage
Amplifier – Input
Ground
Bandwidth control
AGC hold mode
Figure 2. Pinning
IN
SB
A ferrite antenna is connected between IN and VCC. For
high sensitivity, the Q factor of the antenna circuit should
be as high as possible. Please note that a high Q factor
requires temperature compensation of the resonant
frequency in most cases. Specifications are valid for
Q>30. An optimal signal-to-noise ratio will be achieved
by a resonant resistance of 50 to 200 k.
A resistor RSB is connected between SB and GND. It
controls the bandwidth of the crystal filters. It is recommended: RSB = 0 for DCF 77.5 kHz, RSB = 10 k for
60 kHz WWVB and RSB = open for JG2AS 40 kHz.
VCC
SB
IN
GND
Figure 3.
2 (18)
Figure 4.
Rev. A7, 06-Mar-01
U4223B
Q1A, Q1B
SL
In order to achieve a high selectivity, a crystal is connected between the Pins Q1A and Q1B. It is used with the
serial resonant frequency of the time-code transmitter
(e.g., 60 kHz WWVB, 77.5 kHz DCF or 40 kHz JG2AS).
AGC hold mode: SL high (VSL = VCC) sets normal function, SL low (VSL = 0) disconnects the rectifier and holds
the voltage VINT at the integrator output and also the AGC
amplifier gain.
The equivalent parallel capacitor of the filter crystal is
internally compensated. The compensated value is about
0.7 pF. If full sensitivity and selectivity are not needed,
the crystal filter can be substituted by a capacitor of 82 pF.
VCC
SL
Q1B
Q1A
Figure 8.
GND
Figure 5.
INT
REC
Rectifier output and integrator input: The capacitor C1
between REC and INT is the lowpass filter of the rectifier
and at the same time a damping element of the gain
control.
Integrator output: The voltage VINT is the control voltage
for the AGC. The capacitor C2 between INT and DEC
defines the time constant of the integrator. The current
through the capacitor is the input signal of the decoder.
INT
REC
GND
GND
Figure 9.
Figure 6.
FLA, FLB
DEC
Decoder input: Senses the current through the integration
capacitor C2. The dynamic input resistance has a value of
about 420 k and is low compared to the impedance of
C2 .
DEC
Lowpass filter: A capacitor C3 connected between FLA
and FLB suppresses higher frequencies at the trigger
circuit of the decoder.
FLB
FLB
GND
Figure 7.
Rev. A7, 06-Mar-01
94 8377
Figure 10.
3 (18)
U4223B
Q2A, Q2B
According to Q1A/Q1B, a crystal is connected between
the Pins Q2A and Q2B. It is used with the serial resonant
frequency of the time-code transmitter (e.g., 60 kHz
WWVB, 77.5 kHz DCF or 40 kHz JG2AS). The equivalent parallel capacitor of the filter crystal is internally
compensated. The value of the compensation is about
0.7 pF.
Q2A
A sequence of the digitalized time-code signal can be
analyzed by a special noise-suppressing algorithm in
order to increase the sensitivity and the signal-to-noise
ratio (more than 10 dB compared to conventional
decoding). Details about the time-code format are
described separately.
Decimal
0
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
Q2B
GND
Figure 11.
PON
If PON is connected to GND, the receiver will be
activated. The set-up time is typically 0.5 s after applying
GND at this pin. If PON is connected to VCC, the receiver
will switch to power-down mode.
Gray
0000
0001
0011
0010
0110
0111
0101
0100
1100
1101
1111
1110
1010
1011
1001
1000
VCC
VCC
PON
D0 ... D3
PON
GND
Figure 13.
Figure 12.
CLK
D0, D1, D2, D3
The outputs of the ADC consist of PNP-NPN push-pull
stages and can be directly connected to a microcomputer.
In order to avoid any interference of the output into the
antenna circuit, we recommend terminating each digital
output with a capacitor of 10 nF. The digitalized signal of
the ADC is Gray coded (see table). It should be taken into
account that in power-down mode (PON = high), D0, D1,
D2 and D3 will be high.
4 (18)
The input of the ADC is switched to the AGC voltage by
the rising slope of the clock. When conversion time has
passed (about 1.8 ms at 25°C), the digitalized fieldstrength signal is stored in the output registers D0 to D3
as long as the clock is high and can be read by a microcomputer. The falling slope of the clock switches the
input of the ADC to the time-code signal. In the meantime, the digitalized time-code signal is stored in the
output registers D0 to D3 as long as the clock is low (see
figure 14).
Rev. A7, 06-Mar-01
U4223B
Vclk
mV
100
50
0
4
7 8
11 12 t/ms
Now, the time-code
signal can be read
Falling edge initiates
time-code conversion
Now, the AGC value can be read
Thus, the first step in designing the antenna circuit is to
measure the bandwidth. Figure 17 shows an example for
the test circuit. The RF signal is coupled into the bar
antenna by inductive means, e.g., a wire loop. It can be
measured by a simple oscilloscope using the 10:1 probe.
The input capacitance of the probe, typically about 10 pF,
should be taken into consideration. By varying the frequency of the signal generator, the resonant frequency
can be determined.
RF signal
generator
77.5 kHz
Rising edge initiates
AGC signal conversion
Scope
Probe
10 : 1
10 M
Figure 14.
In order to minimize interferences, we recommend a
voltage swing of about 100 mV. A full supply-voltage
swing is possible but reduces the sensitivity.
Cres
Figure 16.
At the point where the voltage of the RF signal at the
probe drops by 3 dB, the two frequencies can then be
measured. The difference between these two frequencies
is called the bandwidth BWA of the antenna circuit. As the
value of the capacitor Cres in the antenna circuit is known,
it is easy to compute the resonant resistance according to
the following formula:
VCC
CLK
R res GND
Figure 15.
Please note:
The signals and voltages at the Pins REC, INT, FLA,
FLB, Q1A, Q1B, Q2A and Q2B cannot be measured by
standard measurement equipment due to very high internal impedances. For the same reason, the PCB should be
protected against surface humidity.
Design Hints for the Ferrite Antenna
The bar antenna is a very critical device of the complete
clock receiver. Observing some basic RF design rules
helps to avoid possible problems. The IC requires a resonant resistance of 50 k to 200 k. This can be achieved
by a variation of the L/C-relation in the antenna circuit.
It is not easy to measure such high resistances in the RF
region. A more convenient way is to distinguish between
the different bandwidths of the antenna circuit and to calculate the resonant resistance afterwards.
Rev. A7, 06-Mar-01
wire loop
1
2 BW A Cres
where
Rres is the resonant resistance,
BWA is the measured bandwidth (in Hz)
Cres is the value of the capacitor in the antenna circuit
(in Farad).
If high inductance values and low capacitor values are
used, the additional parasitic capacitances of the coil
(20 pF) must be considered. The Q value of the capacitor should be no problem if a high Q type is used. The
Q value of the coil differs more or less from the DC
resistance of the wire. Skin effects can be observed but do
not dominate.
Therefore, it should not be a problem to achieve the
recommended values of the resonant resistance. The use
of thicker wire increases the Q value and accordingly
reduces bandwidth. This is advantageous in order to
improve reception in noisy areas. On the other hand,
temperature compensation of the resonant frequency
might become a problem if the bandwidth of the antenna
circuit is low compared to the temperature variation of the
resonant frequency. Of course, the Q value can also be
reduced by a parallel resistor.
5 (18)
U4223B
Temperature compensation of the resonant frequency is
a must if the clock is used at different temperatures.
Please ask your supplier of bar antenna material and of
capacitors for specified values of the temperature
coefficient.
or to use a twisted wire for the antenna-coil connection.
This twisted line is also necessary to reduce feedback of
noise from the microprocessor to the IC input. Long
connection lines must be shielded.
Furthermore, some critical parasitics have to be considered. These are shortened loops (e.g., in the ground line
of the PCB board) close to the antenna and undesired
loops in the antenna circuit. Shortened loops decrease the
Q value of the circuit. They have the same effect like conducting plates close to the antenna. To avoid undesired
loops in the antenna circuit, it is recommended to mount
the capacitor Cres as close as possible to the antenna coil
A final adjustment of the time-code receiver can be
carried out by pushing the coil along the bar antenna. The
maximum of the integrator output voltage VINT at
Pin INT indicates the resonant point. But attention: The
load current should not exceed 1 nA, that means an input
resistance 1 G of the measuring device is required.
Therefore, a special DVM or an isolation amplifier is
necessary.
Absolute Maximum Ratings
Parameters
Supply voltage
Ambient temperature range
Storage temperature range
Junction temperature
Electrostatic handling
(MIL Standard 883 D), except Pins 2, 5, 6, 14 and 15
Symbol
VCC
Tamb
Rstg
Tj
± VESD
Value
5.25
–40 to +85
–40 to +85
125
2000
Unit
V
C
C
C
V
Symbol
RthJA
Maximum
70
Unit
K/W
Thermal Resistance
Parameters
Thermal resistance
Electrical Characteristics
VCC = 3 V, reference point Pin 3, input signal frequency 80 kHz, Tamb = 25C, unless otherwise specified
Parameters
Supply voltage range
Supply current
Test Conditions / Pin
Pin 1
Pin 1
Without reception signal
with reception signal = 200 V
OFF mode
Set-up time after VCC ON
VCC = 1.5 V
AGC amplifier input; IN Pin 2
Reception frequency range
Minimum input voltage
Rres = 100 k, Qres > 30
Maximum input voltage
Input capacitance to GND
6 (18)
Symbol
VCC
ICC
Min
1.2
Typ
15
t
fin
Vin
Vin
Cin
Max
5.25
Unit
V
30
25
0.1
A
A
A
s
80
1.5
kHz
V
mV
pF
2
40
40
1
80
1.5
Rev. A7, 06-Mar-01
U4223B
Parameters
Test Conditions / Pin
ADC; D0, D1, D2, D3
Pins 17, 18, 19 and 20
Output voltage HIGH
RLOAD = 870 k to GND
LOW
RLOAD = 650 k to VCC
Output current HIGH
VTCO = VCC/2
LOW
VTCO = VCC/2
Input current into DEC
Falling slope of CLK
(first bit)
Input current into DEC
Falling slope of CLK
(last bit)
Input current into DEC
Falling slope of CLK
(step range)
Input voltage at IN
RF generator at IN, without
(first bit)
modulation rising slope of CLK
Input voltage at IN
RF generator at IN, without
(last bit)
modulation rising slope of CLK
Input voltage at IN
RF generator at IN, without
(step range)
modulation rising slope of CLK
Clock input; CLK
Pin 12
Input voltage swing
Clock frequency
Dynamical input resistance
Power-ON/OFF control; PON Pin 16
Input voltage
HIGH
Required IIN 0.5 A
LOW
Input current
VCC = 3 V
VCC = 1.5 V
VCC = 5 V
Set-up time after PON
AGC hold mode; SL
Pin 13
Input voltage
HIGH
Required IIN 0.5 A
LOW
Input current
Vin = VCC
Vin = GND
Rejection of interference
fd – fud = 625 Hz
signals
Vd = 3 V, fd = 77.5 kHz
using 2 crystal filters
using 1 crystal filter
Rev. A7, 06-Mar-01
Symbol
Min
Typ
Max
VOH
VOL
VCC-0.4
ISOURCE
ISINK
Idecs
3
4
–24
10
12
–17
–11
V
V
nA
Idece
28
35
42
nA
Idecst
1.75
3.5
7
nA
0.4
Unit
Vmin
–10
dBV
Vmax
75
dBV
Vstep
5.5
dBV
Vswing
fclk
Rdyn.
50
100
100
100
VCC
125
VCC-0.2
IIN
1.4
t
1.7
0.7
3
0.5
VCC-1.2
2
2
VCC-0.2
V
V
A
A
A
s
2.5
V
V
A
A
43
22
dB
dB
VCC-1.2
0.1
af
af
mV
Hz
k
7 (18)
U4223B
Test Circuit (for Fundamental Function)
Test point: DVM with high and
low input line for measuring a
voltage Vxx or a current Ixx
by conversion into a voltage
Ipon
Vd
1.657V
300k
300k
300k
Sd1
Sd2
Sd3
Sd0
Vd0
Vd1
Vd2
Spon
1M
Vd3
D2
D1
300k
PON
D3
Q2B
ÎÎ
Isl
Q2A
Ssl
SL
U4223B
ANALOG
DIGITAL
CONVERTER
TIME
CONTROL
D0
Ivcc
1M
82p
1M
Iclk
CLK
100k
Vclk
VCC
FLB
STABILISATION
DECODING
Iin
Sdec
FLA
AGC–
AMPLIFIER
100M
RECTIFIER
DEC
IN
1M
10M
GND
Q1A
SB
Vcc
3V
Q1B
82p
~
INT
680p
Vrec
Vin
REC
Idec
3.3n
Vdec
420k
Srec
Ssb
Sint
Vsb
10M
10M
Vint
1M
Vrec
Isb
Irec
Vint
Iint
Figure 17. Test circuit
8 (18)
Rev. A7, 06-Mar-01
U4223B
12
ÎÎÎ
ÎÎÎ
10
Field strength
Value ADC
8
6
4
ÎÎÎ
Time-code signal
2
0
80
0
20
40
60
80
0
20
40
60
20
40
60
Time (Gating100/s)
Figure 18. Example of a normal DCF signal
14
ÎÎ
ÎÎ
12
Field strength
Value ADC
10
8
6
ÎÎ
ÎÎ
4
Time-code signal
2
0
80
0
20
40
60
80
0
Time (Gating100/s)
Figure 19. Example of a disturbed DCF signal
Rev. A7, 06-Mar-01
9 (18)
U4223B
Application Circuit for DCF 77.5 kHz
Control lines
+VCC
Ferrite
Antenna
fres = 77.5 kHz
1
20
2
19
3
18
4
17
5
16
77.5 kHz 2)
C1
6.8 nF
C2
33 nF
C3
10 nF
D0
10 nF
D1
10 nF
D2
10 nF
U4223B
6
15
7
14
D3
10 nF
PON 3)
77.5 kHz
Microcomputer
8
13
9
12
10
11
Keyboard
CLK 4)
SL 1)
Display
1)
2)
3)
4)
If SL is not used, SL is connected to VCC
77.5-kHz crystal can be replaced by 10 pF
If IC is activated, PON is connected to GND
Voltage swing 100 mVpp at Pin 12
Figure 20.
Application Circuit for WWVB 60 kHz
Control lines
+VCC
Ferrite
Antenna
1
20
2
19
3
18
4
17
5
16
fres = 60 kHz
10 k
C1
15 nF
C2
47 nF
C3
10 nF
D1
10 nF
D2
10 nF
RSB
60 kHz 2)
D0
10 nF
U4223B
6
15
7
14
D3
10 nF
PON 3)
60 kHz
Microcomputer
8
13
9
12
10
11
Keyboard
CLK 4)
SL 1)
Display
1)
2)
3)
4)
If SL is not used, SL is connected to VCC
60-kHz crystal can be replaced by 10 pF
If IC is activated, PON is connected to GND
Voltage swing 100 mVpp at Pin 12
Figure 21.
10 (18)
Rev. A7, 06-Mar-01
U4223B
Application Circuit for JG2AS 40 kHz
+VCC
Ferrite
Antenna
Control lines
1
20
2
19
3
18
4
17
fres = 40 kHz
C1
680 pF
C3
10 nF
D2
10 nF
U4223B
1 M
220 nF
C2
D1
10 nF
D3
10 nF
PON 3)
16
5
40 kHz 2)
D0
10 nF
6
15
7
14
40 kHz
Microcomputer
CLK 4)
SL 1)
8
13
9
12
10
11
Keyboard
Display
R
1)
2)
3)
4)
If SL is not used, SL is connected to VCC
40-kHz crystal can be replaced by 22 pF
If IC is activated, PON is connected to GND
Voltage swing 100 mVpp at Pin 12
Figure 22.
Rev. A7, 06-Mar-01
11 (18)
U4223B
PAD Coordinates
The T4223B
DIE size:
PAD size:
Thickness:
is also available as die for “chip-on-board” mounting.
2.26 x 2.09 mm
100 x 100 m (contact window 88 x 88 m)
300 m 20 m
SYMBOL
IN1
IN
GND
SB
Q1A
Q1B
REC
INT
DEC
FLA
FLB
X-Axis/m
128
128
354
698
1040
1290
1528
1766
2044
2044
2044
Y-Axis/m
832
310
124
128
128
128
128
128
268
676
1072
SYMBOL
CLK
SL
Q2A
Q2B
PON
TCO
D3
D2
D1
D0
VCC
X-Axis/m
2044
2044
2000
1634
1322
1008
696
384
128
128
128
Y-Axis/m
1400
1638
1876
1876
1876
1876
1876
1876
1682
1454
1138
The PAD coordinates are referred to the left bottom point
of the contact window.
PAD Layout
D2
D3
TCO
PON
Q2A
Q2B
D1
SL
CLK
D0
VCC
FLB
T4223B
IN1
FLA
IN
Y Axis
Reference point (%)
GND
SB
Q1A
Q1B
REC
INT
DEC
94 8892
X Axis
Figure 23.
12 (18)
Rev. A7, 06-Mar-01
U4223B
Information on the German Transmitter
Station: DCF 77,
Frequency 77.5 kHz,
Transmitting power 50 kW
Location: Mainflingen/Germany,
Geographical coordinates: 50 0.1’N, 09
Time of transmission: permanent
Time frame 1 minute
Time frame
( index count 1 second )
5
10
20
15
25
30
35
40
0
55
50
45
5
10
R
A1
Z1
Z2
A2
S
1
2
4
8
10
20
40
P1
1
2
4
8
10
20
P2
1
2
4
8
10
20
1
2
4
1
2
4
8
10
1
2
4
8
10
20
40
80
P3
0
00’E
coding
when
required
minutes
Example:19.35 h
s
1
2
seconds 20
21
22
4
23
10
8
24
25
calendar day month
day
of
the
week
hours
20
26
40
27
28
P1
29
year
2
1
30
8
4
31
minutes
32
10
33
20
34
P2
35
hours
Start Bit
Parity Bit P1
Parity Bit P2
Figure 24.
Modulation
The carrier amplitude is reduced to 25% at the beginning
of each second for a period of 100 ms (binary zero) or
200 ms (binary one), except the 59th second.
Time-Code Format (based on
Information of Deutsche Bundespost)
The time-code format consists of 1-minute time frames.
There is no modulation at the beginning of the 59th
second to indicate the switch over to the next 1-minute
Rev. A7, 06-Mar-01
time frame. A time frame contains BCD-coded information of minutes, hours, calendar day, day of the week,
month and year between the 20th second and 58th second
of the time frame, including the start bit S (200 ms) and
parity bits P1, P2 and P3. Furthermore, there are 5 additional bits R (transmission by reserve antenna), A1
(announcement of change-over to summer time), Z1 (during summer time 200 ms, otherwise 100 ms), Z2 (during
standard time 200 ms, otherwise 100 ms) and A2
(announcement of leap second) transmitted between the
15th second and 19th second of the time frame.
13 (18)
U4223B
Information on the British Transmitter
Station: MSF
Frequency 60 kHz
Transmitting power 50 kW
Location: Teddington, Middlesex
Geographical coordinates: 52 22’N, 01 11’W
Time of transmission: permanent, except the first
Tuesday of each month from 10.00 h to 14.00 h.
Time frame 1 minute
Time frame
( index count 1 second)
10
5
15
20
25
35
30
50
45
40
55
0
year
month
Switch over to
the next time frame
day of
hour
month day
of
week
minute
10
minute
identifier
BST
hour + minute
day of week
day + month
year
BST 7 GMT change
impending
Parity
check
bits
1
0
5
0
80
40
20
10
8
4
2
1
10
8
4
2
1
20
10
8
4
2
1
4
2
1
20
10
8
4
2
1
40
20
10
8
4
2
1
0
0
500 ms 500 ms
Example:
March 1993
seconds 17
80
18
40
19
20
8
10
20
21
4
22
2
23
10
1
24
25
8
26
year
4
27
1
2
28
29
30
month
Figure 25.
Modulation
Time-Code Format
The carrier amplitude is switched off at the beginning of
each second for a period of 100 ms (binary zero) or
200 ms (binary one).
The time-code format consists of 1-minute time frames.
A time frame contains BCD–coded information of year,
month, calendar day, day of the week, hours and minutes.
At the switch-over to the next time frame, the carrier
amplitude is switched off for a period of 500 ms.
The prescence of the fast code during the first 500 ms at
the beginning of the minute in not guaranteed. The transmission rate is 100 bits/s and the code contains
information of hour, minute, day and month.
14 (18)
Rev. A7, 06-Mar-01
U4223B
Information on the US Transmitter
Station: WWVB
Frequency 60 kHz
Transmitting power 40 kW
Location: Fort Collins
Geographical coordinates: 40 40’N, 105
Time of transmission: permanent
Time frame 1 minute
Time frame
( index count 1 second)
45
50
55
0
5
10
P0
80
40
20
10
P5
8
4
2
1
40
ADD
SUB
ADD
P4
800
400
200
100
80
40
20
10
P3
8
4
2
1
days
hours
minutes
35
30
25
200
100
20
8
4
2
1
P2
15
20
10
P0
FRM
40
20
10
10
8
4
2
1
P1
5
0
03’W
daylight savings time bits
leap second warning bit
leap year indicator bit
“0” = non leap year
“1” = leap year
UTI UTI
year
sign correction
Example: UTC 18.42 h
Time frame
P0
seconds 0
40 20 10
1
2
3
8
4
5
4
6
2
7
1
8
P1
20 10
8
4
2
1 P2
9 10 11 12 13 14 15 16 17 18 19 20
minutes
Frame-reference marker
hours
Figure 26.
Modulation
Time-Code Format
The carrier amplitude is reduced by 10 dB at the beginning of each second and is restored within 500 ms (binary
one) or within 200 ms (binary zero).
The time-code format consists of 1-minute time frames.
A time frame contains BCD-coded information of
minutes, hours, days and year. In addition, there are
6 position-identifier markers (P0 thru P5) and 1 framereference marker with reduced carrier amplitude of
800 ms duration.
Rev. A7, 06-Mar-01
15 (18)
U4223B
Information on the Japanese Transmitter
Station: JG2AS
Frequency 40 kHz
Transmitting power 10 kW
Location: Sanwa, Ibaraki
Geographical coordinates: 3611’ N, 13951’ E
Time of transmission: permanent
Time frame 1 minute
Time frame
(index count 1 second)
minutes
hours
45
50
55
0
5
10
P0
40
P5
35
80
40
20
10
P3
8
4
2
1
30
ADD
SUB
ADD
P4
8
4
2
1
25
200
10 0
20
8
4
2
1
P2
15
20
10
10
8
4
2
1
P1
5
PO
FRM
40
20
10
0
da ys
code dut1
Example: 18.42 h
Time frame
P0
seconds 59 0
8
40 20 10
1
2
3
4
4
5
6
2
7
1 P1
8
20 10
8
4
2
1 P2
9 10 11 12 13 14 15 16 17 18 19 20
minutes
hours
Frame-reference marker (FRM)
Position-identifier marker P0
Position identifier marker P1
0.5 second: Binary one
0.8 second: Binary zero
0.2 second: Identifier markers P0...P5
0.8 s
0.5 s
“1”
“0”
0.2 s
“P”
Figure 27.
Modulation
Time-Code Format
The carrier amplitude is 100% at the beginning of each
second and is switched off after 500 ms (binary one) or
after 800 ms (binary zero).
The time-code format consists of 1-minute time frames.
A time frame contains BCD-coded information of
minutes, hours and days. In addition, there are 6 positionidentifier markers (P0 thru P5) and 1 frame-reference
markers (FRM) with reduced carrier amplitude of 800 ms
duration.
16 (18)
Rev. A7, 06-Mar-01
U4223B
Package Information
Package SSO20
5.7
5.3
Dimensions in mm
6.75
6.50
4.5
4.3
1.30
0.15
0.15
0.05
0.25
6.6
6.3
0.65
5.85
20
11
technical drawings
according to DIN
specifications
13007
1
Rev. A7, 06-Mar-01
10
17 (18)
U4223B
Ozone Depleting Substances Policy Statement
It is the policy of Atmel Germany GmbH to
1. Meet all present and future national and international statutory requirements.
2. Regularly and continuously improve the performance of our products, processes, distribution and operating systems
with respect to their impact on the health and safety of our employees and the public, as well as their impact on
the environment.
It is particular concern to control or eliminate releases of those substances into the atmosphere which are known as
ozone depleting substances (ODSs).
The Montreal Protocol (1987) and its London Amendments (1990) intend to severely restrict the use of ODSs and forbid
their use within the next ten years. Various national and international initiatives are pressing for an earlier ban on these
substances.
Atmel Germany GmbH has been able to use its policy of continuous improvements to eliminate the use of ODSs listed
in the following documents.
1. Annex A, B and list of transitional substances of the Montreal Protocol and the London Amendments respectively
2. Class I and II ozone depleting substances in the Clean Air Act Amendments of 1990 by the Environmental
Protection Agency (EPA) in the USA
3. Council Decision 88/540/EEC and 91/690/EEC Annex A, B and C (transitional substances) respectively.
Atmel Germany GmbH can certify that our semiconductors are not manufactured with ozone depleting substances
and do not contain such substances.
We reserve the right to make changes to improve technical design and may do so without further notice.
Parameters can vary in different applications. All operating parameters must be validated for each customer
application by the customer. Should the buyer use Atmel Wireless & Microcontrollers products for any unintended
or unauthorized application, the buyer shall indemnify Atmel Wireless & Microcontrollers against all claims,
costs, damages, and expenses, arising out of, directly or indirectly, any claim of personal damage, injury or death
associated with such unintended or unauthorized use.
Data sheets can also be retrieved from the Internet:
http://www.atmel–wm.com
Atmel Germany GmbH, P.O.B. 3535, D-74025 Heilbronn, Germany
Telephone: 49 (0)7131 67 2594, Fax number: 49 (0)7131 67 2423
18 (18)
Rev. A7, 06-Mar-01