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LTC2421/LTC2422
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The selection between CH0 and CH1 is automatic. Initially,
after power-up, a conversion is performed on CH0. For
each subsequent conversion, the input channel selection
is alternated. Embedded within the serial data output is a
status bit indicating which channel corresponds to the
conversion result. If the conversion was performed on
CH0, this bit (Bit 22) is LOW and is HIGH if the conversion
was performed on CH1 (see Figure 33).
There are no extra control or status pins required to per-
form the alternating 2-channel measurements. The
LTC2422 only requires two digital signals (SCK and SDO).
This simplification is ideal for isolated temperature mea-
surements or systems where minimal control signals are
available.
Pseudo Differential Applications
Generally, designers choose fully differential topologies
for several reasons. First, the interface to a 4- or 6-wire
bridge is simple (it is a differential output). Second, they
require good rejection of line frequency noise. Third, they
typically look at a small differential signal sitting on a
large common mode voltage; they need accurate
measurements of the differential signal independent of
the common mode input voltage. Many applications cur-
rently using fully differential analog-to-digital converters
for any of the above reasons may migrate to a pseudo
differential conversion using the LTC2422.
Direct Connection to a Full Bridge
The LTC2422 interfaces directly to a 4- or 6-wire bridge,
as shown in Figure 34. The LTC2422 includes a FS
SET
and
a ZS
SET
for sensing the excitation voltage directly across
the bridge. This eliminates errors due to excitation cur-
rents flowing through parasitic resistors. The LTC2422
also includes two single ended input channels which can
tie directly to the differential output of the bridge. The two
conversion results may be digitally subtracted yielding the
differential result.
The LTC2422’s single ended rejection of line frequencies
(±2%) and harmonics is better than 110dB. Since the
device performs two independent single ended conver-
sions each with >110dB rejection, the overall common
mode and differential rejection is much better than the
80dB rejection typically found in other differential input
delta-sigma converters.
In addition to excellent rejection of line frequency noise,
the LTC2422 also exhibits excellent single ended noise
rejection over a wide range of frequencies due to its 4
th
order sinc filter. Each single ended conversion indepen-
dently rejects high frequency noise (>60Hz). Care must be
taken to insure noise at frequencies below 15Hz and at
multiples of the ADC sample rate (15,360Hz) are not
present. For this application, it is recommended the
LTC2422 is placed in close proximity to the bridge sensor
in order to reduce the noise injected into the ADC input. By
performing three successive conversions (CH0-CH1-CH0),
the drift and low frequency noise can be measured and
compensated for digitally.
Figure 33. Embedded Selected Channel Indicator
24212 F33
SCK
SDO
CH1
• • • • • •
CH1 DATA OUT
CH0 DATA OUT
EOC
CH0
EOC
Figure 34. Pseudo Differential Strain Guage Application
V
CC
LTC2422
FS
SET
ZS
SET
SCK
CH1
SDO
F
O
CS
CH0
GND
3-WIRE
SPI INTERFACE
1
5V
9
8
7
10
6
24212 F32
2
350 350
350 350
3
4
5
I
DC
= 0
I
EXCITATION
I
DC
= 0
29
LTC2421/LTC2422
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The absolute accuracy (less than 10 ppm total error) of the
LTC2422 enables extremely accurate measurement of
small signals sitting on large voltages. Each of the two
pseudo differential measurements performed by the
LTC2422 is absolutely accurate independent of the com-
mon mode voltage output from the bridge. The pseudo
differential result obtained from digitally subtracting the
two single ended conversion results is accurate to within
the noise level of the device (3µV
RMS
) times the square
root of 2, independent of the common mode input voltage.
Typically, a bridge sensor outputs 2mV/V full scale. With
a 5V excitation, this translates to a full-scale output of
10mV. Divided by the RMS noise of 8.4µV(= 6µV • 1.414),
this circuit yields 1190 counts with no averaging or ampli-
fication. If more counts are required, several conversions
may be averaged (the number of effective counts is in-
creased by a factor of square root of 2 for each doubling
of averages).
An RTD Temperature Digitizer
RTDs used in remote temperature measurements often
have long lead lengths between the ADC and RTD sensor.
These long lead lengths lead to voltage drops due to exci-
tation current in the interconnect to the RTD. This voltage
drop can be measured and digitally removed using the
LTC2422 (see Figure 35).
The excitation current (typically 200µA) flows from the
ADC through a long lead length to the remote temperature
sensor (RTD). This current is applied to the RTD, whose
resistance changes as a function of temperature (100 to
400 for 0°C to 800°C). The same excitation current flows
back to the ADC ground and generates another voltage
drop across the return leads. In order to get an accurate
measurement of the temperature, these voltage drops must
be measured and removed from the conversion result.
Assuming the resistance is approximately the same for the
forward and return paths (R1 = R2), the auxiliary channel
on the LTC2422 can measure this drop. These errors are
then removed with simple digital correction.
The result of the first conversion on CH0 corresponds to an
input voltage of V
RTD
+ R1 • I
EXCITATION.
The result of the
second conversion (CH1) is –R1 • I
EXCITATION.
Note, the
LTC2422’s input range is not limited to the supply rails, it
has underrange capabilities. The device’s input range is
300mV to V
REF
+ 300mV. Adding the two conversion
results together, the voltage drop across the RTD’s leads
are cancelled and the final result is V
RTD
.
An Isolated, 20-Bit Data Acquisition System
The LTC1535 is useful for signal isolation. Figure 36 shows
a fully isolated, 20-bit differential input A/D converter imple-
mented with the LTC1535 and LTC2422. Power on the
isolated side is regulated by an LT1761-5.0 low noise, low
dropout micropower regulator. Its output is suitable for
driving bridge circuits and for ratiometric applications.
During power-up, the LTC2422 becomes active at V
CC
=
2.3V, while the isolated side of the LTC1535 must wait for
V
CC2
to reach its undervoltage lockout threshold of 4.2V.
Figure 35. RTD Remote Temperature Measurement
V
CC
LTC2422
FS
SET
ZS
SET
SCK
CH0
SDO
F
O
CS
CH1
GND
3-WIRE
SPI INTERFACE
1
5V
9
8
7
10
6
24212 F35
2
4
3
+
V
RTD
P
t
100
5
I
DC
= 0
I
EXCITATION
= 200µA
I
EXCITATION
= 200µA
R2
R1
5k
25
1000pF
5k25
0.1µF
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LTC2421/LTC2422
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+
+
F
O
SCK
SDO
CS
GND
V
CC
FS
SET
CH1
CH0
ZS
SET
LTC2422
24212 F36
LT1761-5
GND
10µF
10V
TANT
10µF
10V
TANT
+
10µF
16V
TANT
+
10µF
10V
TANT
10µF
1µF
T1
1/2 BAT54C
1/2 BAT54C
ISOLATION
BARRIER
= LOGIC COMMON
= FLOATING COMMON
T1 = COILTRONICS CTX02-14659
OR SIEMENS B78304-A1477-A3
1k
2
21 2
1
1
1
2
2
2
2
10µF
CERAMIC
A
B
Y
Z
RO
RE
DE
DI
V
CC2
ST2
G1
V
CC1
G2
ST1
“SDO”
“SCK”
LOGIC 5V
IN OUT
SHDN BYP
LTC1535
Figure 36. Complete, Isolated 20-Bit Data Acquisition System
Below 4.2V, the LTC1535’s driver outputs Y and Z are in a
high impedance state, allowing the 1k pull-down to de-
fine the logic state at SCK. When the LTC2422 first be-
comes active, it samples SCK; a logic “0” provided by the
1k pull-down invokes the external serial clock mode. In
this mode, the LTC2422 is controlled by a single clock line
from the nonisolated side of the barrier, through the
LTC1535’s driver output Y. The entire power-up sequence,
from the time power is applied to V
CC1
until the LT1761’s
output has reached 5V, is approximately 1ms.
Data returns to the nonisolated side through the LTC1535’s
receiver at RO. An internal divider on receiver input B sets
a logic threshold of approximately 3.4V at input A, facili-
tating communications with the LTC2422’s SDO output
without the need for any external components.

LTC2421IMS#PBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Analog to Digital Converters - ADC 20-bit Delta-Sigma ADC in MSOP
Lifecycle:
New from this manufacturer.
Delivery:
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