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AD636 датащи(PDF) 11 Page - Analog Devices

номер детали AD636
подробное описание детали  Low Level, True RMS-to-DC Converter
PDF  16 Pages
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производитель  AD [Analog Devices]
домашняя страница  http://www.analog.com
Logo AD - Analog Devices

AD636 датащи(HTML) 11 Page - Analog Devices

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Data Sheet
AD636
Rev. E | Page 11 of 16
slightly more restricted than in the dual supply connection. The
load resistor, RL, is necessary to provide current sinking capability.
C2
3.3µF
AD636
ABSOLUTE
VALUE
SQUARER
DIVIDER
10kΩ
10kΩ
CURRENT
MIRROR
CAV
BUF
+
20kΩ
NONPOLARIZED
39kΩ
0.1µF
0.1µF
+VS
VOUT
RL
1kΩ TO 10kΩ
VIN
1
2
3
4
5
6
7
14
13
12
11
10
9
8
VIN
NC
–VS
CAV
dB
BUF OUT
BUF IN
NC
NC
NC
COM
RL
IOUT
NC = NO CONNECT
+
Figure 11. Single-Supply Connection (See Text)
CHOOSING THE AVERAGING TIME CONSTANT
The AD636 computes the rms of both ac and dc signals. If the
input is a slowly varying dc voltage, the output of the AD636
tracks the input exactly. At higher frequencies, the average
output of the AD636 approaches the rms value of the input
signal. The actual output of the AD636 differs from the ideal
output by a dc (or average) error and some amount of ripple, as
demonstrated in Figure 12.
TIME
IDEAL
EO
DC ERROR = EO – EO (IDEAL)
AVERAGE EO = EO
DOUBLE-FREQUENCY
RIPPLE
EO
Figure 12. Typical Output Waveform for Sinusoidal Input
The dc error is dependent on the input signal frequency and the
value of CAV. Figure 13 can be used to determine the minimum
value of CAV, which yields a given % dc error above a given
frequency using the standard rms connection.
The ac component of the output signal is the ripple. There are
two ways to reduce the ripple. The first method involves using a
large value of CAV. Because the ripple is inversely proportional
to CAV, a tenfold increase in this capacitance effects a tenfold
reduction in ripple. When measuring waveforms with high crest
factors (such as low duty cycle pulse trains), the averaging time
constant should be at least ten times the signal period. For example,
a 100 Hz pulse rate requires a 100 ms time constant, which
corresponds to a 4 μF capacitor (time constant = 25 ms per μF).
INPUT FREQUENCY (Hz)
100
0.01
1
10
0.1
1
10
100
0.1
0.01
*% dc ERROR + % RIPPLE (PEAK)
1
10
100
1k
10k
100k
VALUES FOR CAV AND
1% SETTLING TIME FOR
STATED % OF READING
AVERAGING ERROR*
ACCURACY ±20% DUE TO
COMPONENT TOLERANCE
Figure 13. Error/Settling Time Graph for Use with the Standard RMS
Connection
The primary disadvantage in using a large CAV to remove ripple
is that the settling time for a step change in input level is
increased proportionately. Figure 13 shows the relationship
between CAV and 1% settling time is 115 ms for each microfarad
of CAV. The settling time is twice as great for decreasing signals
as for increasing signals (the values in Figure 13 are for decreasing
signals). Settling time also increases for low signal levels, as
shown in Figure 14.
rms INPUT LEVEL
10.0
7.5
0
10mV
100mV
1.0
5.0
2.5
1V
1mV
Figure 14. Settling Time vs. Input Level
A better method for reducing output ripple is the use of a post-
filter. Figure 15 shows a suggested circuit. If a single-pole filter
is used (C3 removed, RX shorted), and C2 is approximately
5 times the value of CAV, the ripple is reduced, as shown in
Figure 16, and the settling time is increased. For example, with
CAV = 1 µF and C2 = 4.7 μF, the ripple for a 60 Hz input is
reduced from 10% of reading to approximately 0.3% of reading.
The settling time, however, is increased by approximately a
factor of 3. The values of CAV and C2 can therefore be reduced
to permit faster settling times while still providing substantial
ripple reduction.



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