LTC2411-1IMS#PBF Linear Technology, LTC2411-1IMS#PBF Datasheet - Page 36
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LTC2411-1IMS#PBF
Manufacturer Part Number
LTC2411-1IMS#PBF
Description
IC A/DCONV DIFF INPUT&REF 10MSOP
Manufacturer
Linear Technology
Datasheet
1.LTC2411CMSPBF.pdf
(40 pages)
Specifications of LTC2411-1IMS#PBF
Number Of Bits
24
Sampling Rate (per Second)
6.8
Data Interface
MICROWIRE™, Serial, SPI™
Number Of Converters
2
Power Dissipation (max)
1mW
Voltage Supply Source
Single Supply
Operating Temperature
-40°C ~ 85°C
Mounting Type
Surface Mount
Package / Case
10-TFSOP, 10-MSOP (0.118", 3.00mm Width)
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Available stocks
Company
Part Number
Manufacturer
Quantity
Price
APPLICATIO S I FOR ATIO
LTC2411/LTC2411-1
bridge output can be eliminated completely; if the refer-
ence arm of the bridge is used as the reference to the ADC,
as shown in Figure 43. The LTC2411/LTC2411-1 can
accept inputs up to 1/2 V
R1 must be at least 2 the highest value of the variable
resistor.
In the case of 100 platinum RTD’s, this would suggest a
value of 800
advisable due to self-heating effects. A value of 25.5k is
shown for R1, reducing self-heating effects to acceptable
levels for most sensors.
The basic circuit shown in Figure 43 shows connections
for a full 4-wire connection to the sensor, which may be
located remotely. The differential input connections will
reject induced or coupled 60Hz interference, however, the
reference inputs do not have the same rejection. If 60Hz or
other noise is present on the RTD, a low pass filter is
recommended as shown in Figure 44. Note that you
cannot place a large capacitor directly at the junction of R1
and R2, as it will store charge from the sampling process.
A better approach is to produce a low pass filter decoupled
from the input lines with a high value resistor (R3).
The use of a third resistor in the half bridge, between the
variable and fixed elements gives essentially the same
36
for R1. Such a low value for R1 is not
PLATINUM
U
100
RTD
REF
Figure 44. Remote Half Bridge Sensing with Noise Suppression on Reference
U
1
2
. Hence, the reference resistor
3
4
10k, 5%
W
R1
0.1%
10k
R2
10k
5%
R3
U
1 F
–
+
LTC1050
result as the two resistor version, but has a few benefits.
If, for example, a 25k reference resistor is used to set the
excitation current with a 100
reference input is sampling the same external node as the
positive input, but may result in errors if used with a long
cable. For short cable applications, the errors may be
acceptably low. If instead the single 25k resistor is
replaced with a 10k 5% and a 10k 0.1% reference
resistor, the noise level introduced at the reference, at
least at higher frequencies, will be reduced. A filter can be
introduced into the network, in the form of one or more
capacitors, or ferrite beads, as long as the sampling
pulses are not translated into an error. The reference
voltage is also reduced, but this is not undesirable, as it
will decrease the value of the LSB, although, not the input
referred noise level.
The circuit shown in Figure 44 shows a more rigorous
example of Figure 43, with increased noise suppression
and more protection for remote applications.
Figure 45 shows an example of gain in the excitation circuit
and remote feedback from the bridge. The LTC1043s
provide voltage multiplication, providing 10V from a 5V
reference with only 1ppm error. The amplifiers are used at
unity-gain and, hence, introduce a very little error due to
5V
560
10k
10k
2
3
4
5
REF
REF
IN
IN
LTC2411-1
+
–
LTC2411/
+
–
GND
V
5V
CC
1
6
2411 F44
RTD, the negative