28
LTC2424/LTC2428
APPLICATIONS INFORMATION
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Figure 29. Sync
4
Filter Rejection
INPUT FREQUENCY
0
–60
–40
0
f
S
= 15,360Hz
24248 F29
–80
100
f
S
/2 f
S
120
140
–20
REJECTION (dB)
In addition to the dynamic reference current, the V
REF
ESD
protection diodes have a temperature dependent leakage
current. This leakage current, nominally 1nA (±10nA max),
results in a fixed full-scale shift of 10µV for a 10k source
resistance.
Antialiasing
One of the advantages delta-sigma ADCs offer over con-
ventional ADCs is on-chip digital filtering. Combined with
a large oversampling ratio, the LTC2424/LTC2428 signifi-
cantly simplify antialiasing filter requirements.
The digital filter provides very high rejection except at
integer multiples of the modulator sampling frequency
(f
S
), see Figure 29. The modulator sampling frequency is
256 • F
O
, where F
O
is the notch frequency (typically 50Hz
or 60Hz). The bandwidth of signals not rejected by the
digital filter is narrow (0.2%) compared to the bandwidth
of the frequencies rejected.
As a result of the oversampling ratio (256) and the digital
filter, minimal (if any) antialias filtering is required in front
of the LTC2424/LTC2428. If passive RC components are
placed in front of the LTC2424/LTC2428, the input dy-
namic current should be considered. In cases where large
effective RC time constants are used, an external buffer
amplifier may be required to minimize the effects of input
dynamic current.
The modulator contained within the LTC2424/LTC2428
can handle large-signal level perturbations without satu-
rating. Signal levels up to 40% of V
REF
do not saturate the
analog modulator. These signals are limited by the input
ESD protection to 300mV below ground and 300mV above
V
CC
.
Figure 27. INL Error vs R
VREF
(Small C)
Figure 28. INL Error vs R
VREF
(Large C)
RESISTANCE AT V
REF
()
1
30
40
50
1k 10k
24248 F27
20
10
10 100 100k
0
–10
–20
INL ERROR (ppm)
V
CC
= 5V
V
REF
= 5V
T
A
= 25°C
C
VREF
= 0.01µF
C
VREF
= 1000pF
C
VREF
= 0pF
C
VREF
= 100pF
RESISTANCE AT V
REF
()
0
6
8
10
600 800
24248 F28
4
2
–2
–4
–6
–8
–10
200 400 1000
0
INL ERROR (ppm)
C
VREF
= 22µF
C
VREF
= 10µF
C
VREF
= 1µF
C
VREF
= 0.1µF
C
VREF
= 0.01µF
C
VREF
= 0.001µF
V
CC
= 5V
V
REF
= 5V
T
A
= 25°C
Using a Low Power Precision Reference
The circuit in Figure 30 shows the connections and by-
passing for an LT1461-2.5 as a 2.5V reference. The
LT1461 is a bandgap reference capable of 3ppm/°C tem-
perature stability yet consumes only 45µA of current. The
1k resistor between the reference and the ADC reduces the
transient load changes associated with sampling and
produces optimal results. This reference will not impact
the noise level of the LTC2424/LTC2428 if signals are less
29
LTC2424/LTC2428
than 60% full scale, and only marginally increases noise
approaching full scale. Even lower power references can
be used if only the lower end of the LTC2424/LTC2428
input range is required.
2.051MHz Oscillator for 100sps Output Ratio
The oscillator circuit shown in Figure 31 can be used to
drive the F
O
pin, boosting the conversion rate of the
LTC2420 for applications that do not require a notch at 50
or 60Hz. This oscillator is not sensitive to hysteresis
voltage of a Schmitt trigger device as are simpler
relaxation oscillators using the 74HC14 or similar de-
vices. The circuit can be tuned over a 3-1 range with only
one resistor and can be gated. The use of transmission
gates could be used to shift the frequency in order to
provide setable conversion rates.
Pseudodifferential Multichannel Bridge Digitizer and
Digital Cold Junction Compensation
The circuit shown in Figure 32 enables pseudodifferential
measurements of several bridge transducers and abso-
lute temperature measurement.
APPLICATIONS INFORMATION
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Consecutive readings are performed on each side of the
bridge by selecting the appropriate channel on the
LTC2428. Each output is digitized and the results digitally
subtracted to obtain the pseudodifferential result. Several
bridge transducers may be digitized in this manner.
In order to measure absolute temperature with a thermo-
couple, cold junction compensation must be performed.
Channel 6 measures the output of the thermocouple while
channel 7 measures the output of the cold junction sensor
(diode, thermistor, etc.). This enables digital cold junction
compensation of the thermocouple output. The tempera-
ture measurement may then be used to compensate the
temperature effects of the bridge transducers.
THERMOCOUPLE
THERMISTOR
24248 F32
CH0
CH1
CH2
CH3
CH4
CH5
CH6
CH7
9
10
11
12
13
14
15
17
8-CHANNEL
MUX
5ZS
SET
GND
1, 6, 16, 18, 22, 27, 28
23
20
25
19
21
24
CSADC
CSMUX
SCK
CLK
D
IN
SDO
26
F
O
LTC2428
ADCINMUXOUT
7 4 3 2, 8
1µF
5V
5V
FS
SET
V
CC
V
CC
+
20-BIT
Σ ADC
Figure 32. Pseudodifferential Multichannel Bridge Digitizer and Digital Cold Junction Compensation
+
LT1461-2.5
GND
IN
24248 F30
10µF
16V
TANT
TO
LTC2424/LTC2428
FS
SET
OUT5V
1k
0.1µF
CER
Figure 30. Low Power Reference
U1-A U1-B U1-C
U1-F
U1-E
TO LTC2424/
LTC2428
F
O
PIN
U1-D
12
5pF
5k
1k
2N3904
10k
47k
1k
47k
10pF
100smps, F
O
= 2.048MHz
30smps, F
O
= 614.4kHz
U1: 74HC14 OR EQUIVALENT
270pF
345 6
12 13
HALT
11 10
9 8
24248 F31
Figure 31. 2.051MHz Oscillator for 100sps Output Rate
30
LTC2424/LTC2428
The LTC2428’s Resolution and Accuracy Allows You
to Measure Points in a Ladder of Sensors
In many industrial processes, for example, cracking tow-
ers in petroleum refineries, a group of temperature mea-
surements must be related to one another. A series of
platinum RTDs that sense slow changing temperatures
can be configured into a resistive ladder, using the LTC2428
to sense each node. This approach allows a single excita-
tion current passed through the entire ladder, reducing
total supply current consumption. In addition, this ap-
proach requires only one high precision resistor, thereby
reducing cost. A group of up to seven temperatures can be
measured as a group by a single LTC2428 in a loop-pow-
ered remote acquisition unit. In the example shown in
Figure 33, the excitation current is 240µA at 0°C. The
LTC2428 requires 300µA, leaving nearly 3.5mA for the
remainder of the remote transmitter.
The resistance of any of the RTDs (PT1 to PT7) is deter-
mined from the voltage across it, as compared to the
voltage drop across the reference resistor (R1). This is a
ratiometric implementation where the voltage drop across
R1 is given by V
REF
– V
CH1
. Channel 7 is used to measure
the voltage on a representative length of wire. If the same
type and length of wire is used for all connections, then
errors associated with the voltage drops across all wiring
can be removed in software. The contribution of wiring
drop can be scaled if wire lengths are not equal.
Gain can be added to this circuit as the total voltage drop
across all the RTDs is small compared to ADC full-scale
range. The maximum recommended gain is 50, as limited
by both amplifier noise contribution, as well as the maxi-
mum voltage developed at CH0 when all sensors are at the
maximum temperature specified for platinum RTDs.
24248 F33
CH0
CH1
CH2
CH3
CH4
CH5
CH6
CH7
9
10
11
12
13
14
15
17
8-CHANNEL
MUX
5ZS
SET
GND
1, 6, 16, 18, 22, 27, 28
23
20
25
19
21
24
CSADC
CSMUX
SCK
CLK
D
IN
SDO
26
F
O
LTC2428
ADCINMUXOUT
74
7
0.1µF
6
3
6
47µF
R2300µA
5V
45
OPTIONAL
GAIN
BLOCK
2
TO PT3-PT6
PT1
100
PLATINUM
RTD
OPTIONAL
PROTECTION
RESISTORS
5k MAX
UP TO SEVERAL
HUNDRED FEET.
ALL SAME
WIRE TYPE
PT2
PT7
4
R3
5V
R2
R1
20.1k
0.1%
3 2, 8
1µF
5V
FS
SET
V
CC
V
CC
+
+
LTC1050
LTC1634-2.5
+
20-BIT
Σ ADC
Figure 33. Measuring Up to Seven RTD Temperatures with One Reference Resistor and One Reference Current
APPLICATIONS INFORMATION
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LTC2424CG#TRPBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Analog to Digital Converters - ADC 4/Ch 20-Bit Delta Sigma ADC
Lifecycle:
New from this manufacturer.
Delivery:
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