LTC1967IMS8TR Linear Technology, LTC1967IMS8TR Datasheet - Page 10
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LTC1967IMS8TR
Manufacturer Part Number
LTC1967IMS8TR
Description
Manufacturer
Linear Technology
Datasheet
1.LTC1967IMS8TR.pdf
(28 pages)
Specifications of LTC1967IMS8TR
Operating Temperature (min)
-40C
Operating Temperature (max)
85C
Operating Temperature Classification
Industrial
Mounting
Surface Mount
Pin Count
8
Package Type
MSOP
Lead Free Status / RoHS Status
Not Compliant
APPLICATIO S I FOR ATIO
LTC1967
Because this peak has energy (proportional to voltage
squared) that is 16 times (4
the peak is necessarily present for at most 6.25% (1/16)
of the time.
The LTC1967 performs very well with crest factors of 4 or
less and will respond with reduced accuracy to signals
with higher crest factors. The high performance with crest
factors less than 4 is directly attributable to the high
linearity throughout the LTC1967.
DESIGN COOKBOOK
The LTC1967 RMS-to-DC converter makes it easy to
implement a rather quirky function. For many applications
all that will be needed is a single capacitor for averaging,
appropriate selection of the I/O connections and power
supply bypassing. Of course, the LTC1967 also requires
power. A wide variety of power supply configurations are
shown in the Typical Applications section towards the end
of this data sheet.
Capacitor Value Selection
The RMS or root-mean-squared value of a signal, the root
of the mean of the square , cannot be computed without
some averaging to obtain the mean function. The LTC1967
true RMS-to-DC converter utilizes a single capacitor on
the output to do the low frequency averaging required for
RMS-to-DC conversion. To give an accurate measure of a
dynamic waveform, the averaging must take place over a
sufficiently long interval to average, rather than track, the
10
–0.2
–0.4
–0.6
–0.8
–1.6
–1.8
–2.0
–1.0
–1.2
–1.4
0
1
C = 10 F
C = 4.7 F
U
C = 2.2 F
C = 22 F
U
2
) the energy of the RMS value,
W
C = 1 F
Figure 6. DC Error vs Input Frequency
U
INPUT FREQUENCY (Hz)
C = 0.47 F
10
lowest frequency signals of interest. For a single averaging
capacitor, the accuracy at low frequencies is depicted in
Figure 6.
Figure 6 depicts the so-called “DC error” that results at a
given combination of input frequency and filter capacitor
values
the output is fed to a circuit with an inherently band-limited
frequency response, such as a dual slope/integrating A/D
converter, a
meter.
However, if the output is examined on an oscilloscope with
a very low frequency input, the incomplete averaging will
be seen, and this ripple will be larger than the error
depicted in Figure 6. Such an output is depicted in
Figure 7. The ripple is at twice the frequency of the input
2
therefore easy to trim or calibrate out. The “Error Analyses” section to follow discusses the effect
of static error terms.
This frequency-dependent error is in additon to the static errors that affect all readings and are
2
. It is appropriate for most applications, in which
Figure 7. Output Ripple Exceeds DC Error
C = 0.22 F
ACTUAL OUTPUT
WITH RIPPLE
f = 2 f
RIPPLE
A/D converter or even a mechanical analog
PEAK
(5%)
INPUT
PEAK RIPPLE
DC ERROR +
ERROR =
(5.05%)
PEAK
TIME
(0.05%)
ERROR
DC
C = 0.1 F
OUTPUT
IDEAL
OF ACTUAL
AVERAGE
OUTPUT
DC
1967 F07
1967 F06
100
1967f