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參數(shù)資料
| 型號(hào)： | T4223B-MF |
| 廠商： | ATMEL CORP |
| 元件分類： | 消費(fèi)家電 |
| 英文描述： | Time-Code Receiver with A/D Converter |
| 中文描述： | SPECIALTY CONSUMER CIRCUIT, UUC22 |
| 封裝： | DIE-22 |
| 文件頁數(shù)： | 5/18頁 |
| 文件大?。?/td> | 138K |
| 代理商： | T4223B-MF |
U4223B
Rev. A7, 06-Mar-01
5 (18)
0
4
8
12
t/ms
50
100
V
clk
mV
7
11
Now, the time-code
signal can be read
Falling edge initiates
time-code conversion
Now, the AGC value can be read
Rising edge initiates
AGC signal conversion
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.
CLK
GND
VCC
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 inter-
nal 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 reso-
nant 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 cal-
culate the resonant resistance afterwards.
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 fre-
quency of the signal generator, the resonant frequency
can be determined.
Scope
RF signal
generator
77.5 kHz
C
res
Probe
10 : 1
10 M
wire loop
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 BW
A
of the antenna circuit. As the
value of the capacitor C
res
in the antenna circuit is known,
it is easy to compute the resonant resistance according to
the following formula:
1
2
BW
A
where
R
res
is the resonant resistance,
BW
A
is the measured bandwidth (in Hz)
C
res
is the value of the capacitor in the antenna circuit
(in Farad).
R
res
C
res
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 capa-
citor 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.
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