LTC2413IGN [Linear]
24-Bit No Latency ADC, with Simultaneous 50Hz/60Hz Rejection; 24位无延迟的ADC ,具有同时抑制50Hz / 60Hz抑制型号: | LTC2413IGN |
厂家: | Linear |
描述: | 24-Bit No Latency ADC, with Simultaneous 50Hz/60Hz Rejection |
文件: | 总44页 (文件大小:453K) |
中文: | 中文翻译 | 下载: | 下载PDF数据表文档文件 |
LTC2413
24-Bit No Latency ∆ΣTM ADC,
with Simultaneous 50Hz/60Hz Rejection
U
DESCRIPTIO
FEATURES
The LTC®2413 is a 2.7V to 5.5V simultaneous 50Hz/60Hz
rejection micropower 24-bit differential ∆Σ analog to
digital converter with an integrated oscillator, 2ppm INL
and 0.16ppm RMS noise. It uses delta-sigma technology
and provides single cycle settling time for multiplexed
applications. Through a single pin, the LTC2413 can be
configured for better than 87dB input differential mode
rejection over the range of 49Hz to 61.2Hz (50Hz and
60Hz ±2% simultaneously), or it can be driven by an
external oscillator for a user defined rejection frequency.
The internal oscillator requires no external frequency
setting components.
■
Simultaneous 50Hz/60Hz Rejection
(87dB Minimum)
Differential Input and Differential Reference with
GND to VCC Common Mode Range
2ppm INL and No Missing Codes at 24 Bits
0.1ppm Offset and 2.5ppm Full-Scale Error
0.16ppm Noise
No Latency: Digital Filter Settles in a Single Cycle.
Internal Oscillator—No External Components
Required
24-Bit ADC in Narrow SSOP-16 Package
(SO-8 Footprint)
■
■
■
■
■
■
■
■
■
■
Single Supply 2.7V to 5.5V Operation
Low Supply Current (200µA) and Auto Shutdown
Pin Compatible with LTC2410
The converter accepts any external differential reference
voltage from 0.1V to VCC for flexible ratiometric and
remote sensing measurement configurations. The full-
U
scale differential input range is from –0.5VREF to 0.5VREF
.
APPLICATIO S
The reference common mode voltage, VREFCM, and the
input common mode voltage, VINCM, may be indepen-
dently set anywhere within the GND to VCC range of the
LTC2413. The DC common mode input rejection is better
than 140dB.
■
Direct Sensor Digitizer
■
Weight Scales
■
Direct Temperature Measurement
Gas Analyzers
Strain-Gauge Transducers
■
■
The LTC2413 communicates through a flexible 3-wire
digital interface which is compatible with SPI and
MICROWIRETM protocols.
■
Instrumentation
Data Acquisition
Industrial Process Control
6-Digit DVMs
■
■
, LTC and LT are registered trademarks of Linear Technology Corporation.
No Latency ∆Σ is a trademark of Linear Technology Corporation.
MICROWIRE is a trademark of National Semiconductor Corporation.
■
■
Products for International Markets
U
TYPICAL APPLICATIO
Measured Noise Rejection from 48Hz to 62.5Hz
–80
MEASURED DATA
CALCULATED DATA
–85
–90
2.7V TO 5.5V
1µF
= EXTERNAL CLOCK SOURCE
= INTERNAL OSC/
2
14
13
V
F
O
CC
LTC2413
–95
SIMULTANEOUS 50Hz/60Hz REJECTION
–100
–105
–110
–115
–120
3
4
+
REFERENCE
VOLTAGE
REF
REF
SCK
–
0.1V TO V
CC
3-WIRE
SPI INTERFACE
5
6
12
11
+
ANALOG INPUT RANGE
–0.5V TO 0.5V
IN
SDO
CS
REF
REF
–
IN
1, 7, 8, 9, 10, 15, 16
GND
48
50
52
54
56
58
60
62
2413 TA01
INPUT FREQUENCY (Hz)
2413 TA02
sn2413 2413fs
1
LTC2413
W W U W
U
W
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ABSOLUTE AXI U RATI GS
PACKAGE/ORDER I FOR ATIO
(Notes 1, 2)
TOP VIEW
ORDER PART NUMBER
Supply Voltage (VCC) to GND.......................–0.3V to 7V
Analog Input Pins Voltage
to GND.................................... –0.3V to (VCC + 0.3V)
Reference Input Pins Voltage
to GND.................................... –0.3V to (VCC + 0.3V)
Digital Input Voltage to GND........ –0.3V to (VCC + 0.3V)
Digital Output Voltage to GND ..... –0.3V to (VCC + 0.3V)
Operating Temperature Range
LTC2413C ............................................... 0°C to 70°C
LTC2413I............................................ –40°C to 85°C
Storage Temperature Range ................. –65°C to 150°C
Lead Temperature (Soldering, 10 sec).................. 300°C
1
2
3
4
5
6
7
8
16
15
14
13
12
11
10
9
GND
GND
GND
V
CC
LTC2413CGN
LTC2413IGN
+
F
O
REF
–
SCK
SDO
CS
REF
+
IN
GN PART MARKING
–
IN
GND
GND
GND
GND
2413
2413I
GN PACKAGE
16-LEAD PLASTIC SSOP
TJMAX = 125°C, θJA = 95°C/W
Consult factory for parts specified with wider operating temperature ranges.
ELECTRICAL CHARACTERISTICS
The ● denotes specifications which apply over the full operating
temperature range, otherwise specifications are at TA = 25°C. (Notes 3, 4)
PARAMETER
CONDITIONS
≤ V , –0.5 • V ≤ V ≤ 0.5 • V , (Note 5)
MIN
TYP
MAX
UNITS
Resolution (No Missing Codes) 0.1V ≤ V
●
●
●
24
Bits
REF
CC
REF
IN
REF
+
–
Integral Nonlinearity
4.5V ≤ V ≤ 5.5V, REF = 2.5V, REF = GND, V
= 1.25V, (Note 6)
= 2.5V, (Note 6)
1
2
5
ppm of V
ppm of V
ppm of V
CC
INCM
REF
REF
REF
+
–
5V ≤ V ≤ 5.5V, REF = 5V, REF = GND, V
REF = 2.5V, REF = GND, V
14
CC
INCM
+
–
= 1.25V, (Note 6)
INCM
+
–
Offset Error
2.5V ≤ REF ≤ V , REF = GND,
0.5
2.5
µV
CC
+
–
GND ≤ IN = IN ≤ V , (Note 13)
CC
+
–
Offset Error Drift
2.5V ≤ REF ≤ V , REF = GND,
10
nV/°C
ppm of V
CC
+
–
GND ≤ IN = IN ≤ V
CC
+
–
Positive Full-Scale Error
Positive Full-Scale Error Drift
Negative Full-Scale Error
Negative Full-Scale Error Drift
Total Unadjusted Error
2.5V ≤ REF ≤ V , REF = GND,
●
●
2.5
12
12
CC
REF
+
+
–
+
IN = 0.75 • REF , IN = 0.25 • REF
+
–
2.5V ≤ REF ≤ V , REF = GND,
0.03
2.5
ppm of V /°C
REF
CC
+
+
–
+
+
+
IN = 0.75 • REF , IN = 0.25 • REF
+
–
2.5V ≤ REF ≤ V , REF = GND,
ppm of V
REF
CC
+
+
–
IN = 0.25 • REF , IN = 0.75 • REF
+
–
2.5V ≤ REF ≤ V , REF = GND,
0.03
ppm of V /°C
REF
CC
+
+
–
IN = 0.25 • REF , IN = 0.75 • REF
+
–
4.5V ≤ V ≤ 5.5V, REF = 2.5V, REF = GND, V
5V ≤ V ≤ 5.5V, REF = 5V, REF = GND, V
REF = 2.5V, REF = GND, V
= 1.25V
= 2.5V
3
3
4
ppm of V
ppm of V
ppm of V
CC
INCM
REF
REF
REF
+
–
CC
INCM
+
–
= 1.25V
INCM
+
Output Noise
5V ≤ V ≤ 5.5V, REF = 5V, V – = GND,
0.8
µV
RMS
CC
REF
–
+
GND ≤ IN = IN ≤ 5V, (Note 12)
sn2413 2413fs
2
LTC2413
U
CO VERTER CHARACTERISTICS
The ● denotes specifications which apply over the full operating
temperature range, otherwise specifications are at TA = 25°C. (Notes 3, 4)
PARAMETER
CONDITIONS
MIN
TYP
MAX
UNITS
+
–
Input Common Mode Rejection DC 2.5V ≤ REF ≤ V , REF = GND,
●
●
●
●
●
●
130
140
dB
CC
–
+
GND ≤ IN = IN ≤ V
CC
+
–
Input Common Mode Rejection
49Hz to 61.2Hz
2.5V ≤ REF ≤ V , REF = GND,
140
87
dB
dB
dB
dB
dB
CC
–
+
GND ≤ IN = IN ≤ V , (Note 7)
CC
Input Normal Mode Rejection
49Hz to 61.2Hz
(Note 7)
Input Normal Mode Rejection
External Oscillator
External Oscillator
87
External Clock f
/2560 ±14%
EOSC
Input Normal Mode Rejection
External Clock f /2560 ±4%
110
130
140
140
EOSC
+
–
Reference Common Mode
Rejection DC
2.5V ≤ REF ≤ V , GND ≤ REF ≤ 2.5V,
CC
–
+
V
= 2.5V, IN = IN = GND
REF
+
–
–
+
Power Supply Rejection, DC
REF = 2.5V, REF = GND, IN = IN = GND
120
120
dB
dB
+
–
Power Supply Rejection
Simultaneous 50Hz/60Hz ±2%
REF = 2.5V, REF = GND,
–
+
IN = IN = GND, (Note 7)
U
U
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A ALOG I PUT A D REFERE CE The ● denotes specifications which apply over the full operating
temperature range, otherwise specifications are at TA = 25°C. (Note 3)
SYMBOL
PARAMETER
CONDITIONS
MIN
TYP
MAX
UNITS
+
+
IN
Absolute/Common Mode IN Voltage
●
●
●
GND – 0.3V
GND – 0.3V
V
V
+ 0.3V
V
V
V
CC
CC
–
–
IN
Absolute/Common Mode IN Voltage
+ 0.3V
/2
V
Input Differential Voltage Range
–V /2
REF
V
IN
REF
+
–
(IN – IN )
+
–
+
REF
REF
Absolute/Common Mode REF Voltage
●
●
●
0.1
GND
0.1
V
V
V
V
CC
–
Absolute/Common Mode REF Voltage
V
– 0.1V
CC
V
Reference Differential Voltage Range
V
CC
REF
+
–
(REF – REF )
+
+
C (IN )
IN Sampling Capacitance
18
18
18
18
1
pF
pF
pF
pF
nA
nA
nA
nA
S
–
–
C (IN )
IN Sampling Capacitance
S
+
+
C (REF )
REF Sampling Capacitance
S
–
–
C (REF )
REF Sampling Capacitance
S
+
+
+
I
I
I
I
(IN )
IN DC Leakage Current
CS = V , IN = GND
●
●
●
●
–10
–10
–10
–10
10
DC_LEAK
DC_LEAK
DC_LEAK
DC_LEAK
CC
–
–
–
(IN )
IN DC Leakage Current
CS = V , IN = GND
1
10
10
10
CC
+
+
+
(REF )
REF DC Leakage Current
CS = V , REF = 5V
1
CC
–
–
–
(REF )
REF DC Leakage Current
CS = V , REF = GND
1
CC
sn2413 2413fs
3
LTC2413
U
U
DIGITAL I PUTS A D DIGITAL OUTPUTS
The ● denotes specifications which apply over the full
operating temperature range, otherwise specifications are at TA = 25°C. (Note 3)
SYMBOL
PARAMETER
CONDITIONS
2.7V ≤ V ≤ 5.5V
MIN
TYP
MAX
UNITS
V
IH
V
IL
V
IH
V
IL
High Level Input Voltage
●
●
●
●
●
●
2.5
2.0
V
V
CC
CS, F
2.7V ≤ V ≤ 3.3V
O
CC
Low Level Input Voltage
CS, F
4.5V ≤ V ≤ 5.5V
0.8
0.6
V
V
CC
2.7V ≤ V ≤ 5.5V
O
CC
High Level Input Voltage
SCK
2.7V ≤ V ≤ 5.5V (Note 8)
2.5
2.0
V
V
CC
2.7V ≤ V ≤ 3.3V (Note 8)
CC
Low Level Input Voltage
SCK
4.5V ≤ V ≤ 5.5V (Note 8)
0.8
0.6
V
V
CC
2.7V ≤ V ≤ 5.5V (Note 8)
CC
I
I
Digital Input Current
0V ≤ V ≤ V
CC
–10
–10
10
µA
µA
pF
pF
V
IN
IN
CS, F
O
Digital Input Current
SCK
0V ≤ V ≤ V (Note 8)
10
IN
IN
CC
C
C
V
V
V
V
Digital Input Capacitance
10
10
IN
CS, F
O
Digital Input Capacitance
SCK
(Note 8)
IN
High Level Output Voltage
SDO
I = –800µA
O
●
●
●
●
●
V
V
– 0.5V
– 0.5V
OH
OL
OH
OL
CC
CC
Low Level Output Voltage
SDO
I = 1.6mA
O
0.4
V
High Level Output Voltage
SCK
I = –800µA (Note 9)
O
V
Low Level Output Voltage
SCK
I = 1.6mA (Note 9)
O
0.4
10
V
I
Hi-Z Output Leakage
SDO
–10
µA
OZ
W U
POWER REQUIRE E TS
The ● denotes specifications which apply over the full operating temperature range,
otherwise specifications are at TA = 25°C. (Note 3)
SYMBOL
PARAMETER
Supply Voltage
Supply Current
CONDITIONS
MIN
TYP
MAX
UNITS
V
CC
●
2.7
5.5
V
I
CC
Conversion Mode
Sleep Mode
CS = 0V (Note 11)
●
●
200
20
300
30
µA
µA
CS = V (Note 11)
CC
sn2413 2413fs
4
LTC2413
W U
TI I G CHARACTERISTICS
The ● denotes specifications which apply over the full operating temperature
range, otherwise specifications are at TA = 25°C. (Note 3)
SYMBOL
PARAMETER
CONDITIONS
MIN
2.56
0.25
0.25
TYP
MAX
2000
390
UNITS
kHz
µs
f
t
t
t
External Oscillator Frequency Range
External Oscillator High Period
External Oscillator Low Period
Conversion Time
●
●
●
EOSC
HEO
390
µs
LEO
F = 0V
●
●
146.71
EOSC
ms
ms
CONV
O
External Oscillator (Note 10)
20510/f
(in kHz)
f
Internal SCK Frequency
Internal Oscillator (Note 9)
External Oscillator (Notes 9, 10)
17.5
kHz
kHz
ISCK
f
/8
EOSC
D
Internal SCK Duty Cycle
(Note 9)
(Note 8)
(Note 8)
(Note 8)
●
●
●
●
45
55
%
kHz
ns
ISCK
f
t
t
t
External SCK Frequency Range
External SCK Low Period
2000
ESCK
250
250
1.80
LESCK
External SCK High Period
ns
HESCK
DOUT_ISCK
Internal SCK 32-Bit Data Output Time
Internal Oscillator (Notes 9, 11)
External Oscillator (Notes 9, 10)
●
●
1.83
1.86
ms
ms
256/f
(in kHz)
EOSC
t
t
External SCK 32-Bit Data Output Time
CS ↓ to SDO Low Z
CS ↑ to SDO Hi-Z
(Note 8)
●
●
●
●
●
●
●
●
●
32/f
(in kHz)
ms
ns
ns
ns
ns
ns
ns
ns
ns
DOUT_ESCK
1
ESCK
0
0
200
200
200
t2
t3
t4
CS ↓ to SCK ↓
(Note 9)
(Note 8)
0
CS ↓ to SCK ↑
50
t
t
SCK ↓ to SDO Valid
SDO Hold After SCK ↓
SCK Set-Up Before CS ↓
SCK Hold After CS ↓
220
50
KQMAX
KQMIN
(Note 5)
15
50
t
t
5
6
Note 1: Absolute Maximum Ratings are those values beyond which the
life of the device may be impaired.
Note 7: FO = 0V (internal oscillator) or fEOSC = 139800Hz ±2%
(external oscillator).
Note 2: All voltage values are with respect to GND.
Note 8: The converter is in external SCK mode of operation such that
the SCK pin is used as digital input. The frequency of the clock signal
driving SCK during the data output is fESCK and is expressed in kHz.
Note 3: VCC = 2.7V to 5.5V unless otherwise specified.
VREF = REF+ – REF–, VREFCM = (REF+ + REF–)/2;
V
IN = IN+ – IN–, VINCM = (IN+ + IN–)/2.
Note 9: The converter is in internal SCK mode of operation such that
the SCK pin is used as digital output.
Note 10: The external oscillator is connected to the FO pin. The external
Note 4: FO pin tied to GND or to external conversion clock source with
EOSC = 139800Hz unless otherwise specified.
f
oscillator frequency, fEOSC, is expressed in kHz.
Note 5: Guaranteed by design, not subject to test.
Note 11: The converter uses the internal oscillator. FO = 0V.
Note 12: The output noise includes the contribution of the internal
calibration operations.
Note 13: Guaranteed by design and test correlation.
Note 6: Integral nonlinearity is defined as the deviation of a code from
a straight line passing through the actual endpoints of the transfer
curve. The deviation is measured from the center of the quantization
band.
sn2413 2413fs
5
LTC2413
U W
TYPICAL PERFOR A CE CHARACTERISTICS
Total Unadjusted Error vs
Temperature (VCC = 5V,
Total Unadjusted Error vs
Temperature (VCC = 5V,
VREF = 2.5V)
Total Unadjusted Error vs
Temperature (VCC = 2.7V,
VREF = 2.5V)
VREF = 5V)
1.5
1.0
1.5
1.0
10
8
V
= 5V
CC
+
REF = 2.5V
–
REF = GND
6
V
V
= 2.5V
INCM
= GND
REF
4
T
= 90°C
= 1.25V
A
0.5
0.5
F
O
2
T = 25°C
A
T
T
T
= 90°C
= 25°C
= –45°C
0
0
A
A
A
0
T
T
= 90°C
= 25°C
–2
–4
–6
–8
–10
A
–0.5
–1.0
–1.5
–0.5
–1.0
–1.5
A
T
= –45°C
V
V
= 2.5V
INCM
= GND
A
REF
T
= –45°C
A
= 1.25V
F
O
–2.5 –2 –1.5 –1 –0.5
V
0
0.5
1
1.5
2
2.5
–1
–0.5
0
0.5
1
–1
–0.5
0
0.5
1
(V)
V
(V)
V
(V)
IN
IN
IN
2413 G01
2413 G02
2413 G03
Integral Nonlinearity vs
Temperature (VCC = 5V,
VREF = 2.5V)
Integral Nonlinearity vs
Temperature (VCC = 5V,
VREF = 5V)
Integral Nonlinearity vs
Temperature (VCC = 2.7V,
VREF = 2.5V)
1.5
1.0
1.5
1.0
10
8
V
= 2.7V
V
V
F
= 2.5V
REF
CC
V
= 5V
+
REF = 2.5V
= 1.25V
INCM
–
REF = GND
= GND
O
6
T
= –45°C
= 25°C
A
T
= 25°C
A
T
4
A
0.5
0.5
T
= 90°C
2
A
0
0
0
T
A
= 90°C
–2
–4
–6
–8
–10
T
= 90°C
= 25°C
REF = 2.5V
A
A
–0.5
–1.0
–1.5
–0.5
–1.0
–1.5
–
REF = GND
T
T
V
V
F
= 2.5V
INCM
= GND
REF
= 1.25V
= –45°C
A
O
–2.5 –2 –1.5 –1 –0.5
V
0
0.5
1
1.5
2
2.5
–1
–0.5
0
0.5
1
–1
–0.5
0
0.5
1
(V)
V
(V)
V
(V)
IN
IN
IN
2413 G04
2413 G05
2413 G06
Noise Histogram (Output Rate =
6.83Hz, VCC = 5V, VREF = 5V)
Noise Histogram (Output Rate =
22.5Hz, VCC = 5V, VREF = 5V)
Noise Histogram (Output Rate =
52.5Hz, VCC = 5V, VREF = 5V)
12
10
8
12
10
8
12
10
8
10,000 CONSECUTIVE
READINGS
GAUSSIAN
10,000 CONSECUTIVE
READINGS
GAUSSIAN
10,000 CONSECUTIVE
READINGS
GAUSSIAN
DISTRIBUTION
m = 0.105ppm
σ = 0.153ppm
DISTRIBUTION
m = 0.067ppm
σ = 0.151ppm
DISTRIBUTION
m = 8.285ppm
σ = 0.311ppm
V
V
V
= 5V
V
V
V
= 5V
V
V
V
= 5V
CC
REF
IN
CC
REF
IN
CC
REF
= 5V
= 5V
= 5V
= 0V
= 0V
= 0V
IN
+
+
+
–
REF = 5V
REF = 5V
REF = 5V
–
–
REF = GND
REF = GND
REF = GND
+
–
+
–
+
–
IN = 2.5V
IN = 2.5V
IN = 2.5V
6
6
6
IN = 2.5V
IN = 2.5V
IN = 2.5V
F
= GND
= 25°C
F
= 460800Hz
= 25°C
F = 1075200Hz
O
O
O
T
T
T = 25°C
A
A
A
4
4
4
2
2
2
0
0
0
–0.8 –0.6 –0.4 –0.2
0
0.2 0.4 0.6 0.8
–0.8 –0.6 –0.4 –0.2
0
0.2 0.4 0.6 0.8
–9.8 –9.4 –9 –8.6 –8.2 –7.8 –7.4 –7 –6.6
OUTPUT CODE (ppm OF V
)
OUTPUT CODE (ppm OF V
)
OUTPUT CODE (ppm OF V
)
REF
REF
REF
sn2413 2413fs
2413 G07
2413 G08
2413 G09
6
LTC2413
U W
TYPICAL PERFOR A CE CHARACTERISTICS
Noise Histogram (Output Rate =
6.83Hz VCC = 5V, VREF = 2.5V)
Noise Histogram (Output Rate =
22.5Hz, VCC = 5V, VREF = 2.5V)
Noise Histogram (Output Rate =
52.5Hz, VCC = 5V, VREF = 2.5V)
12
10
8
12
10
8
12
10
8
10,000 CONSECUTIVE
READINGS
GAUSSIAN
10,000 CONSECUTIVE
READINGS
GAUSSIAN
10,000 CONSECUTIVE
READINGS
GAUSSIAN
DISTRIBUTION
m = 0.033ppm
σ = 0.293ppm
DISTRIBUTION
m = 0.014ppm
σ = 0.292ppm
DISTRIBUTION
m = 3.852ppm
σ = 0.326ppm
V
V
V
= 5V
V
V
V
= 5V
V
V
V
= 5V
CC
REF
IN
CC
REF
IN
CC
REF
= 2.5V
= 2.5V
= 2.5V
= 0V
= 0V
= 0V
IN
+
+
+
–
REF = 2.5V
REF = 2.5V
REF = 2.5V
–
–
REF = GND
REF = GND
REF = GND
+
–
+
–
+
–
IN = 1.25V
IN = 1.25V
IN = 1.25V
6
6
6
IN = 1.25V
IN = 1.25V
IN = 1.25V
F
= GND
= 25°C
F
= 460800Hz
= 25°C
F = 1075200Hz
O
O
O
T
T
T = 25°C
A
A
A
4
4
4
2
2
2
0
0
0
–1.6
–0.8
0
0.8
1.6
–1.6 –1.2 –0.8 –0.4
0
0.4 0.8 1.2 1.6
–5.5 –5.1 –4.7 –4.3 –3.9 –3.5 –3.1 –2.7 –2.3
OUTPUT CODE (ppm OF V
)
OUTPUT CODE (ppm OF V
)
OUTPUT CODE (ppm OF V
)
REF
REF
REF
2413 G10
2413 G11
2413 G12
Noise Histogram (Output Rate =
22.5Hz, VCC = 2.7V, VREF = 2.5V)
Noise Histogram (Output Rate =
6.83Hz VCC = 2.7V, VREF = 2.5V)
Noise Histogram (Output Rate =
52.5Hz, VCC = 2.7V, VREF = 2.5V)
12
10
8
12
10
8
10
9
8
7
6
5
4
3
2
1
0
10,000 CONSECUTIVE
READINGS
GAUSSIAN
10,000 CONSECUTIVE
READINGS
GAUSSIAN
10,000 CONSECUTIVE
READINGS
GAUSSIAN
DISTRIBUTION
m = 0.079ppm
σ = 0.298ppm
DISTRIBUTION
m = 0.177ppm
σ = 0.297ppm
DISTRIBUTION
m = 3.714ppm
σ = 1.295ppm
V
V
V
= 2.7V
V
V
V
= 2.7V
V
V
V
= 2.7V
CC
REF
IN
CC
REF
IN
CC
REF
= 2.5V
= 2.5V
= 2.5V
= 0V
= 0V
= 0V
IN
+
+
+
–
REF = 2.5V
REF = 2.5V
REF = 2.5V
–
–
REF = GND
REF = GND
REF = GND
+
–
+
–
+
–
IN = 1.25V
IN = 1.25V
IN = 1.25V
6
6
IN = 1.25V
IN = 1.25V
IN = 1.25V
F
= GND
= 25°C
F
= 460800Hz
= 25°C
F = 1075200Hz
O
A
O
A
O
T
T
T = 25°C
A
4
4
2
2
0
0
–1.6 –1.2 –0.8 –0.4
0
0.4 0.8 1.2 1.6
–1.6 –1.2 –0.8 –0.4
0
0.4 0.8 1.2 1.6
–10 –8.5 –7 –5.5 –4 –2.5 –1 0.5
OUTPUT CODE (ppm OF V
2
OUTPUT CODE (ppm OF V
)
OUTPUT CODE (ppm OF V
)
)
REF
REF
REF
2413 G13
2413 G14
2413 G15
Long-Term Noise Histogram
(Time = 60 Hrs, VCC = 5V,
VREF = 5V)
Consecutive ADC Readings vs
Time
RMS Noise vs Input Differential
Voltage
12
10
8
1.0
0.8
0.5
0.4
0.3
0.2
0.1
0
GAUSSIAN DISTRIBUTION
m = 0.101837ppm
V
V
= 5V
CC
= 5V
REF
σ = 0.154515ppm
+
REF = 5V
0.6
–
REF = GND
0.4
ADC CONSECUTIVE
READINGS
V
= 2.5V
= GND
= 25°C
INCM
F
O
0.2
V
V
V
= 5V
= 5V
T
CC
REF
IN
A
6
0
= 0V
+
–0.2
–0.4
–0.6
–0.8
–1.0
REF = 5V
–
4
REF = GND
+
–
IN = 2.5V
+
–
V
V
V
= 5V
T = 25°C
A
IN = 2.5V
CC
IN = 2.5V
+
= 5V REF = 5V IN = 2.5V
2
REF
F
= GND
= 25°C
–
O
A
= 0V REF = GND
IN
T
F
= GND
O
0
–0.8 –0.6 –0.4 –0.2
0
0.2 0.4 0.6 0.8
0
5
10 15 20 25 30 35 40 45 50 55 60
TIME (HOURS)
–2.5 –2 –1.5 –1 –0.5
0
0.5
1
1.5
2
2.5
OUTPUT CODE (ppm OF V
)
INPUT DIFFERENTIAL VOLTAGE (V)
REF
2413 G16
2413 G17
sn241234123 4G1183fs
7
LTC2413
U W
TYPICAL PERFOR A CE CHARACTERISTICS
RMS Noise vs VINCM
RMS Noise vs Temperature (TA)
RMS Noise vs VCC
850
825
800
775
750
725
700
675
650
850
825
800
775
750
725
700
675
650
850
825
800
775
750
725
700
675
650
+
–
REF = 2.5V
V
= 5V
CC
+
REF = GND
REF = 5V
–
V
= 2.5V
REF
REF = GND
+
+
–
IN = GND
IN = 2.5V
–
IN = GND
IN = 2.5V
F
= GND
O
A
V
F
= 0V
= GND
IN
O
T
= 25°C
V
= 5V
CC
+
REF = 5V
–
REF = GND
V
= 5V
REF
+
–
IN = V
INCM
INCM
IN = V
V
= 0V
IN
F
= GND
O
T
= 25°C
A
–0.5 0 0.5
1
1.5
2
2.5
3
(V)
3.5
4
4.5
5
5.5
–50
–25
0
25
50
75
100
2.7 3.1 3.5 3.9 4.3 4.7 5.1 5.5
(V)
V
INCM
TEMPERATURE (°C)
V
CC
2413 G19
2413 G20
2413 G21
Offset Error vs VINCM
RMS Noise vs VREF
Offset Error vs Temperature (TA)
850
825
800
775
750
725
700
675
650
0.3
0.2
0.3
0.2
V
= 5V
CC
–
REF = GND
+
–
IN = GND
IN = GND
F
= GND
= 25°C
O
A
0.1
0.1
T
V
= 5V
CC
+
REF = 5V
0
0
–
V
= 5V
REF = GND
CC
+
REF = 5V
V
= 5V
REF
–
+
–
REF = GND
IN = V
–0.1
–0.2
–0.3
–0.1
–0.2
–0.3
INCM
INCM
+
–
IN = 2.5V
IN = V
IN = 2.5V
V
F
A
= 0V
IN
O
V
F
= 0V
= GND
= GND
IN
O
T
= 25°C
0
0.5
1
1.5
2
V
2.5
(V)
3
3.5
4
4.5
5
–0.5 0 0.5
1
1.5
2
2.5
3
(V)
3.5
4
4.5
5
5.5
–50
–25
0
25
50
75
100
V
INCM
TEMPERATURE (°C)
REF
2413 G22
2413 G23
2413 G24
+Full-Scale Error vs
Temperature (TA)
Offset Error vs VCC
Offset Error vs VREF
0.3
0.2
0.3
0.2
3
2
1
0.1
0.1
0
0
0
+
–
REF = 2.5V
V
= 5V
V
= 5V
CC
REF = GND
CC
–
+
REF = GND
REF = 5V
V
= 2.5V
–0.1
–0.2
–0.3
–0.1
–0.2
–0.3
–1
–2
–3
REF
+
–
–
+
IN = GND
IN = GND
REF = GND
IN = GND
+
–
–
IN = 2.5V
IN = GND
F
= GND
= 25°C
IN = GND
F
= GND
O
A
O
A
T
F = GND
T
= 25°C
O
2.7 3.1 3.5 3.9 4.3 4.7 5.1 5.5
(V)
0
0.5
1
1.5
2
V
2.5
(V)
3
3.5
4
4.5
5
–45 –30 –15
0
15 30 45 60 75 90
V
CC
TEMPERATURE (°C)
REF
2413 G25
2413 G26
2413 G27
sn2413 2413fs
8
LTC2413
U W
TYPICAL PERFOR A CE CHARACTERISTICS
–Full-Scale Error vs
Temperature (TA)
+Full-Scale Error vs VCC
+Full-Scale Error vs VREF
3
2
3
2
3
2
V
= 5V
CC
+
REF = 5V
–
REF = GND
+
–
IN = GND
IN = 2.5V
1
1
1
F
= GND
O
0
0
0
+
–
V
= 5V
CC
REF = 2.5V
+
REF = V
REF
REF = GND
–
REF = GND
–1
–2
–3
–1
–2
–3
–1
–2
–3
V
= 2.5V
REF
+
–
+
+
IN = 0.5 • REF
IN = 1.25V
–
IN = GND
IN = GND
F
= GND
= 25°C
O
A
F
= GND
O
A
T
T
= 25°C
2.7 3.1 3.5 3.9 4.3 4.7 5.1 5.5
(V)
0
0.5
1
1.5
2
V
2.5
(V)
3
3.5
4
4.5
5
–45 –30 –15
0
15 30 45 60 75 90
V
TEMPERATURE (°C)
CC
REF
2413 G28
2413 G29
2413 G30
–Full-Scale Error vs VCC
PSRR vs Frequency at VCC
–Full-Scale Error vs VREF
3
2
3
2
0
–20
+
–
V
= 5V
V
= 4.1V ± 1.4V
REF = 2.5V
CC
CC DC
+
+
REF = V
REF = 2.5V
REF = GND
REF
–
–
REF = GND
REF = GND
V
= 2.5V
REF
+
–
+
–
+
IN = GND
IN = GND
IN = GND
–40
+
–
IN = 0.5 • REF
IN = GND
IN = 1.25V
1
1
F
= GND
= 25°C
F
= GND
F
= GND
= 25°C
O
A
O
O
A
–60
T
T
= 25°C
A
T
0
0
–80
–1
–2
–3
–1
–2
–3
–100
–120
–140
2.7 3.1 3.5 3.9 4.3 4.7 5.1 5.5
(V)
0
0.5
1
1.5
2
V
2.5
(V)
3
3.5
4
4.5
5
0.01
0.1
1
10
100
V
FREQUENCY AT V (Hz)
CC
CC
REF
2413 G31
2413 G32
2413 G33
PSRR vs Frequency at VCC
PSRR vs Frequency at VCC
PSRR vs Frequency at VCC
0
–20
0
0
–20
+
–
V
= 4.1V ± 1.4V
REF = 2.5V
V
= 4.1V ± 0.7V
CC
DC
CC DC
+
+
REF = 2.5V
REF = GND
REF = 2.5V
–20
–40
–
+
–
–
REF = GND
IN = GND
REF = GND
+
–
+
–
IN = GND
IN = GND
IN = GND
–40
–40
IN = GND
F
= GND
IN = GND
O
A
F
= GND
= 25°C
T
= 25°C
F = GND
O
A
O
–60
–60
–60
T
T
A
= 25°C
–80
–80
–80
–100
–120
–140
–100
–120
–140
–100
–120
–140
0
20 40 60 80 100 120 140 160 180 200 220
FREQUENCY AT V (Hz)
1
10
100
1k
10k 100k
1M
13900
13950
FREQUENCY AT V (Hz)
14000
14050
14100
FREQUENCY AT V (Hz)
CC
CC
CC
2413 G34
2413 G35
2413 G36
sn2413 2413fs
9
LTC2413
U W
TYPICAL PERFOR A CE CHARACTERISTICS
Conversion Current vs
Temperature (TA)
Conversion Current vs
Output Data Rate
Sleep Current vs Temperature (TA)
220
210
200
190
180
170
160
1100
1000
900
800
700
600
500
400
300
200
100
23
22
21
20
19
18
17
16
F
= GND
V
= 5V
F = GND
O
O
CC
+
CS = GND
SCK = NC
SDO = NC
REF = 5V
CS = V
CC
–
REF = GND
SCK = NC
SDO = NC
+
–
IN = GND
V
= 5.5V
CC
IN = GND
V
V
= 5.5V
= 2.7V
CC
CC
T
= 25°C
= EXTERNAL OSC
A
O
F
V
= 4.1V
CC
CS = GND
SCK = NC
SDO = NC
V
V
= 4.1V
= 2.7V
CC
CC
–45 –30 –15
0
15 30 45 60 75 90
TEMPERATURE (°C)
0
10 20 30 40 50 60 70 80 90 100
OUTPUT DATA RATE (READINGS/SEC) 2413 G38
–45 –30 –15
0
15 30 45 60 75 90
TEMPERATURE (°C)
2413 G37
2413 G39
U
U
U
PI FU CTIO S
GND (Pins 1, 7, 8, 9, 10, 15, 16): Ground. Multiple ground
pins internally connected for optimum ground current flow
and VCC decoupling. Connect each one of these pins to a
groundplanethroughalowimpedanceconnection.Allseven
pins must be connected to ground for proper operation.
SDO (Pin 12): Three-State Digital Output. During the Data
Output period, this pin is used as serial data output. When
the chip select CS is HIGH (CS = VCC), the SDO pin is in a
high impedance state. During the Conversion and Sleep
periods, this pin is used as the conversion status output.
TheconversionstatuscanbeobservedbypullingCSLOW.
VCC (Pin 2): Positive Supply Voltage. Bypass to GND
(Pin 1) with a 10µF tantalum capacitor in parallel with
0.1µF ceramic capacitor as close to the part as possible.
REF+ (Pin 3), REF– (Pin 4): Differential Reference Input.
ThevoltageonthesepinscanhaveanyvaluebetweenGND
and VCC as long as the reference positive input, REF+, is
maintained more positive than the reference negative
input, REF –, by at least 0.1V.
IN+(Pin5), IN–(Pin6):DifferentialAnalogInput. Thevoltage
on these pins can have any value between
GND–0.3VandVCC +0.3V.Withintheselimits, theconverter
bipolar input range (VIN = IN+ – IN–) extends from –0.5 •
(VREF) to 0.5 • (VREF). Outside this input range, the converter
produces unique overrange and underrange output codes.
SCK (Pin 13): Bidirectional Digital Clock Pin. In Internal
Serial Clock Operation mode, SCK is used as digital output
for the internal serial interface clock during the Data
Output period. In External Serial Clock Operation mode,
SCK is used as digital input for the external serial interface
clock during the Data Output period. A weak internal pull-
up is automatically activated in Internal Serial Clock Op-
eration mode. The Serial Clock Operation mode is deter-
mined by the logic level applied to the SCK pin at power up
or during the most recent falling edge of CS.
FO (Pin 14): Frequency Control Pin. Digital input that
controls the ADC’s notch frequencies and conversion
time. When the FO pin is connected to GND (FO = 0V), the
converter uses its internal oscillator and the digital filter
rejects 50Hz and 60Hz simultaneously. When the FO pin is
CS (Pin 11): Active LOW Digital Input. A LOW on this pin
enables the SDO digital output and wakes up the ADC.
Following each conversion, the ADC automatically enters
the Sleep mode and remains in this low power state as
long as CS is HIGH. A LOW-to-HIGH transition on CS
during the Data Output transfer aborts the data transfer
and starts a new conversion.
driven by an external clock signal with a frequency fEOSC
,
the converter uses this signal as its system clock and the
digital filter has 87dB minimum rejection in the range
fEOSC/2560 ±14% and 110dB minimum rejection at
fEOSC/2560 ±4%.
sn2413 2413fs
10
LTC2413
U
U
W
FU CTIO AL BLOCK DIAGRA
INTERNAL
OSCILLATOR
V
CC
GND
AUTOCALIBRATION
AND CONTROL
F
O
(INT/EXT)
+
IN
IN
+
–
–
∫
∫
∫
SDO
SERIAL
INTERFACE
∑
ADC
SCK
CS
+
REF
REF
–
DECIMATING FIR
–
+
DAC
2413 FD
Figure 1. Functional Block Diagram
V
CC
TEST CIRCUITS
1.69k
SDO
SDO
1.69k
C
= 20pF
LOAD
C
= 20pF
LOAD
Hi-Z TO V
OH
OH
V
OL
V
OH
TO V
Hi-Z TO V
OL
OL
TO Hi-Z
V
V
TO V
2413 TA03
OH
OL
TO Hi-Z
2413 TA04
U
W U U
APPLICATIO S I FOR ATIO
CONVERTER OPERATION
CONVERT
Converter Operation Cycle
SLEEP
The LTC2413 is a low power, delta-sigma analog-to-
digitalconverterwithaneasytouse3-wireserialinterface.
Its operation is made up of three states. The converter
operating cycle begins with the conversion, followed by
the low power sleep state and ends with the data output
(see Figure 2). The 3-wire interface consists of serial data
output (SDO), serial clock (SCK) and chip select (CS).
FALSE
CS = LOW
AND
SCK
TRUE
DATA OUTPUT
2413 F02
Initially, the LTC2413 performs a conversion. Once the
conversion is complete, the device enters the sleep state.
Whileinthissleepstate,powerconsumptionisreducedby
an order of magnitude. The part remains in the sleep state
as long as CS is HIGH. The conversion result is held
indefinitely in a static shift register while the converter is
in the sleep state.
Figure 2. LTC2413 State Transition Diagram
sn2413 2413fs
11
LTC2413
U
W U U
APPLICATIO S I FOR ATIO
Once CS is pulled LOW, the device begins outputting the
conversion result. There is no latency in the conversion
result. The data output corresponds to the conversion just
performed. This result is shifted out on the serial data out
pin (SDO) under the control of the serial clock (SCK). Data
is updated on the falling edge of SCK allowing the user to
reliably latch data on the rising edge of SCK (see Figure 3).
The data output state is concluded once 32 bits are read
out of the ADC or when CS is brought HIGH. The device
automatically initiates a new conversion and the cycle
repeats.
TheLTC2413performsoffsetandfull-scalecalibrationsin
every conversion cycle. This calibration is transparent to
the user and has no effect on the cyclic operation de-
scribed above. The advantage of continuous calibration is
extreme stability of offset and full-scale readings with re-
specttotime,supplyvoltagechangeandtemperaturedrift.
Power-Up Sequence
The LTC2413 automatically enters an internal reset state
when the power supply voltage VCC drops below approxi-
mately 2.2V. This feature guarantees the integrity of the
conversion result and of the serial interface mode selec-
tion. (See the 2-wire I/O sections in the Serial Interface
Timing Modes section.)
Through timing control of the CS and SCK pins, the
LTC2413 offers several flexible modes of operation
(internal or external SCK and free-running conversion
modes). These various modes do not require program-
ming configuration registers; moreover, they do not dis-
turbthecyclicoperationdescribedabove. Thesemodesof
operation are described in detail in the Serial Interface
Timing Modes section.
When the VCC voltage rises above this critical threshold,
the converter creates an internal power-on-reset (POR)
signal with a duration of approximately 0.5ms. The POR
signal clears all internal registers. Following the POR
signal, the LTC2413 starts a normal conversion cycle and
followsthesuccessionofstatesdescribedabove. Thefirst
conversion result following POR is accurate within the
specifications of the device if the power supply voltage is
restored within the operating range (2.7V to 5.5V) before
the end of the POR time interval.
Conversion Clock
A major advantage the delta-sigma converter offers over
conventional type converters is an on-chip digital filter
(commonlyimplementedasasincorcombfilter).Forhigh
resolution, low frequency applications, this filter is de-
signed to simultaneously reject line frequencies of 50Hz
and 60Hz plus their harmonics. The filter rejection perfor-
mance is directly related to the accuracy of the converter
system clock. The LTC2413 incorporates a highly accu-
rate on-chip oscillator. This eliminates the need for exter-
nal frequency setting components such as crystals or
oscillators. The LTC2413 achieves a minimum of 87dB
over the range of 49Hz to 61.2Hz.
Reference Voltage Range
This converter accepts a truly differential external refer-
ence voltage. The absolute/common mode voltage speci-
ficationfortheREF+ andREF– pinscoverstheentirerange
from GND to VCC. For correct converter operation, the
REF+ pin must always be more positive than the REF– pin.
The LTC2413 can accept a differential reference voltage
from 0.1V to VCC. The converter output noise is deter-
mined by the thermal noise of the front-end circuits, and
as such, its value in nanovolts is nearly constant with
reference voltage. A decrease in reference voltage will not
significantly improve the converter’s effective resolution.
On the other hand, a reduced reference voltage will im-
prove the converter’s overall INL performance. A reduced
reference voltage will also improve the converter perfor-
mance when operated with an external conversion clock
(external FO signal) at substantially higher output data
Ease of Use
The LTC2413 data output has no latency, filter settling
delay or redundant data associated with the conversion
cycle.Thereisaone-to-onecorrespondencebetweenthe
conversion and the output data. Therefore, multiplexing
multiple analog voltages is easy.
rates (see the Output Data Rate section).
sn2413 2413fs
12
LTC2413
U
W U U
APPLICATIO S I FOR ATIO
Input Voltage Range
This bit is HIGH during the conversion and goes LOW
when the conversion is complete.
The analog input is truly differential with an absolute/
common mode range for the IN+ and IN– input pins
extending from GND – 0.3V to VCC + 0.3V. Outside
these limits, the ESD protection devices begin to turn on
and the errors due to input leakage current increase
rapidly. Within these limits, the LTC2413 converts the
bipolar differential input signal, VIN = IN+ – IN–, from
Bit 30 (second output bit) is a dummy bit (DMY) and is
always LOW.
Bit 29 (third output bit) is the conversion result sign indi-
cator (SIG). If VIN is >0, this bit is HIGH. If VIN is <0, this
bit is LOW.
Bit 28 (fourth output bit) is the most significant bit (MSB)
of the result. This bit in conjunction with Bit 29 also
provides the underrange or overrange indication. If both
Bit 29 and Bit 28 are HIGH, the differential input voltage is
above +FS. If both Bit 29 and Bit 28 are LOW, the
differential input voltage is below –FS.
–FS = –0.5 • VREF to +FS = 0.5 • VREF where VREF
=
REF+ – REF–. Outside this range, the converter indicates
the overrange or the underrange condition using distinct
output codes.
Input signals applied to IN+ and IN– pins may extend by
300mV below ground and above VCC. In order to limit any
fault current, resistors of up to 5k may be added in series
with the IN+ and IN– pins without affecting the perfor-
mance of the device. In the physical layout, it is important
to maintain the parasitic capacitance of the connection
betweentheseseriesresistorsandthecorrespondingpins
as low as possible; therefore, the resistors should be
located as close as practical to the pins. The effect of the
series resistance on the converter accuracy can be evalu-
ated from the curves presented in the Input Current/
Reference Current sections. In addition, series resistors
will introduce a temperature dependent offset error due to
the input leakage current. A 1nA input leakage current will
develop a 1ppm offset error on a 5k resistor if VREF = 5V.
This error has a very strong temperature dependency.
The function of these bits is summarized in Table 1.
Table 1. LTC2413 Status Bits
Bit 31 Bit 30 Bit 29 Bit 28
Input Range
EOC
DMY
SIG MSB
V
≥ 0.5 • V
0
0
0
0
0
1
1
0
0
1
0
1
0
IN
REF
0V ≤ V < 0.5 • V
0
IN
REF
–0.5 • V ≤ V < 0V
0
REF
IN
V
< –0.5 • V
0
IN
REF
Bits 28-5 are the 24-bit conversion result MSB first.
Bit 5 is the least significant bit (LSB).
Bits 4-0 are sub LSBs below the 24-bit level. Bits 4-0 may
be included in averaging or discarded without loss of
resolution.
Output Data Format
DataisshiftedoutoftheSDOpinundercontroloftheserial
clock (SCK), see Figure 3. Whenever CS is HIGH, SDO
remains high impedance and any externally generated
SCK clock pulses are ignored by the internal data out shift
register.
The LTC2413 serial output data stream is 32 bits long. The
first 3 bits represent status information indicating the sign
and conversion state. The next 24 bits are the conversion
result, MSB first. The remaining 5 bits are sub LSBs
beyond the 24-bit level that may be included in averaging
or discarded without loss of resolution. The third and
fourthbitstogetherarealsousedtoindicateanunderrange
condition(thedifferentialinputvoltageisbelow–FS)oran
overrangecondition(thedifferentialinputvoltageisabove
+FS).
In order to shift the conversion result out of the device, CS
mustfirstbedrivenLOW. EOCisseenattheSDOpinofthe
deviceonceCSispulledLOW.EOCchangesrealtimefrom
HIGH to LOW at the completion of a conversion. This
signal may be used as an interrupt for an external
microcontroller. Bit 31 (EOC) can be captured on the first
risingedgeofSCK. Bit30isshiftedoutofthedeviceonthe
first falling edge of SCK. The final data bit (Bit 0) is shifted
Bit 31 (first output bit) is the end of conversion (EOC)
indicator. This bit is available at the SDO pin during the
conversion and sleep states whenever the CS pin is LOW.
out on the falling edge of the 31st SCK and may be latched
sn2413 2413fs
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on the rising edge of the 32nd SCK pulse. On the falling
edgeofthe32ndSCKpulse,SDOgoesHIGHindicatingthe
initiation of a new conversion cycle. This bit serves as EOC
(Bit 31) for the next conversion cycle. Table 2 summarizes
the output data format.
Simultaneous Frequency Rejection
The LTC2413 internal oscillator provides better than 87dB
normalmoderejectionovertherangeof49Hzto61.2Hzas
shown in Figure 4. For this simultaneous 50Hz/60Hz
rejection, FO should be connected to GND.
AslongasthevoltageontheIN+ andIN–pinsismaintained
within the –0.3V to (VCC + 0.3V) absolute maximum
operating range, a conversion result is generated for any
differential input voltage VIN from –FS = –0.5 • VREF to
+FS=0.5•VREF.Fordifferentialinputvoltagesgreaterthan
+FS, the conversion result is clamped to the value corre-
sponding to the +FS + 1LSB. For differential input voltages
below –FS, the conversion result is clamped to the value
corresponding to –FS – 1LSB.
When a fundamental rejection frequency different from
therange49Hzto61.2Hzisrequiredorwhentheconverter
must be sychronized with an outside source, the LTC2413
canoperatewithanexternalconversionclock.Theconveter
automatically detects the presence of an external clock
signal at the FO pin and turns off the internal oscillator. The
frequency fEOSC of the external signal must be at least
2560Hztobedetected.Theexternalclocksignaldutycycle
is not significant as long as the minimum and maximum
specifications for the high and low periods, tHEO and tLEO
,
are observed.
CS
BIT 31
EOC
BIT 30
“0”
BIT 29
SIG
BIT 28
MSB
BIT 27
BIT 5
BIT 0
SDO
SCK
LSB
24
Hi-Z
1
2
3
4
5
26
27
32
SLEEP
DATA OUTPUT
CONVERSION
2413 F03
Figure 3. Output Data Timing
Table 2. LTC2413 Output Data Format
Differential Input Voltage
V *
Bit 31
EOC
Bit 30
DMY
Bit 29
SIG
Bit 28
MSB
Bit 27
Bit 26
Bit 25
…
Bit 0
IN
V * ≥ 0.5 • V **
0
0
0
0
0
0
0
0
0
0
0
0
0
0
0
0
0
0
0
1
1
1
1
1
0
0
0
0
0
1
0
0
0
0
1
1
1
1
0
0
1
1
0
0
1
1
0
0
1
0
1
0
1
0
1
0
1
0
1
0
1
0
1
0
1
0
1
0
1
…
…
…
…
…
…
…
…
…
…
0
1
0
1
0
1
0
1
0
1
IN
REF
0.5 • V ** – 1LSB
REF
0.25 • V **
REF
0.25 • V ** – 1LSB
REF
0
–1LSB
–0.25 • V **
REF
–0.25 • V ** – 1LSB
REF
–0.5 • V **
REF
V * < –0.5 • V **
0
IN
REF
+
–
*The differential input voltage V = IN – IN .
IN
+
–
**The differential reference voltage V = REF – REF .
REF
sn2413 2413fs
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–80
–90
While operating with an external conversion clock of a
frequency fEOSC, the LTC2413 provides better than 110dB
normal mode rejection in a frequency range fEOSC/2560
±4%. The normal mode rejection as a function of the input
frequency deviation from fEOSC/2560 is shown in Figure 5.
–100
–100
–120
–130
–140
Whenever an external clock is not present at the FO pin the
converterautomaticallyactivatesitsinternaloscillatorand
enters the Internal Conversion Clock mode. The LTC2413
operation will not be disturbed if the change of conversion
clock source occurs during the sleep state or during the
data output state while the converter uses an external
serial clock. If the change occurs during the conversion
state, the result of the conversion in progress may be
outside specifications but the following conversions will
notbeaffected.Ifthechangeoccursduringthedataoutput
state and the converter is in the Internal SCK mode, the
serial clock duty cycle may be affected but the serial data
stream will remain valid.
48
50
52
54
56
58
60
62
DIFFERENTIAL INPUT SIGNAL FREQUENCY (Hz)
2413 F04
Figure 4. LTC2413 Normal Mode Rejection
When Using an Internal Oscillator
–80
–85
–90
–95
–100
–105
–110
–115
–120
–125
–130
–135
–140
Table 3 summarizes the duration of each state and the
achievable output data rate as a function of FO.
SERIAL INTERFACE PINS
The LTC2413 transmits the conversion results and re-
ceives the start of conversion command through a syn-
chronous 3-wire interface. During the conversion and
sleep states, this interface can be used to assess the
converter status and during the data output state it is used
to read the conversion result.
–12
–8
–4
0
4
8
12
DIFFERENTIAL INPUT SIGNAL FREQUENCY
DEVIATION FROM NOTCH FREQUENCY f
/2560(%)
2413 F05
EOSC
Figure 5. LTC2413 Normal Mode Rejection When
Using an External Oscillator of Frequency fEOSC
Table 3. LTC2413 State Duration
State
Operating Mode
Duration
CONVERT
Internal Oscillator
F = LOW
Simultaneous 50Hz/60Hz Rejection
147ms, Output Data Rate ≤ 6.8 Readings/s
O
External Oscillator
F = External Oscillator
20510/f
s, Output Data Rate ≤ f
/20510 Readings/s
EOSC
O
EOSC
with Frequency f
kHz
EOSC
(f
EOSC
/2560 Rejection)
SLEEP
As Long As CS = HIGH Until CS = LOW and SCK
DATA OUTPUT
Internal Serial Clock
External Serial Clock with
F = LOW
(Internal Oscillator)
As Long As CS = LOW But Not Longer Than 1.83ms
(32 SCK cycles)
O
F = External Oscillator with
As Long As CS = LOW But Not Longer Than 256/f
ms
EOSC
O
Frequency f
kHz
(32 SCK cycles)
EOSC
As Long As CS = LOW But Not Longer Than 32/f ms
SCK
Frequency f
kHz
(32 SCK cycles)
SCK
sn2413 2413fs
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LTC2413
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Serial Clock Input/Output (SCK)
In addition, the CS signal can be used to trigger a new
conversion cycle before the entire serial data transfer has
been completed. The LTC2413 will abort any serial data
transfer in progress and start a new conversion cycle
anytime a LOW-to-HIGH transition is detected at the CS
pin after the converter has entered the data output state
(i.e., after the first rising edge of SCK occurs with
CS = LOW).
The serial clock signal present on SCK (Pin 13) is used to
synchronizethedatatransfer.Eachbitofdataisshiftedout
the SDO pin on the falling edge of the serial clock.
In the Internal SCK mode of operation, the SCK pin is an
output and the LTC2413 creates its own serial clock by
dividing the internal conversion clock by 8. In the External
SCK mode of operation, the SCK pin is used as input. The
internalorexternalSCKmodeisselectedonpower-upand
then reselected every time a HIGH-to-LOW transition is
detected at the CS pin. If SCK is HIGH or floating at power-
up or during this transition, the converter enters the inter-
nal SCK mode. If SCK is LOW at power-up or during this
transition, the converter enters the external SCK mode.
Finally, CS can be used to control the free-running modes
of operation, see Serial Interface Timing Modes section.
Grounding CS will force the ADC to continuously convert
at the maximum output rate selected by FO. Tying a
capacitor to CS will reduce the output rate and power
dissipation by a factor proportional to the capacitor’s
value, see Figures 13 to 15.
Serial Data Output (SDO)
SERIAL INTERFACE TIMING MODES
The serial data output pin, SDO (Pin 12), provides the
result of the last conversion as a serial bit stream (MSB
first) during the data output state. In addition, the SDO pin
is used as an end of conversion indicator during the
conversion and sleep states.
The LTC2413’s 3-wire interface is SPI and MICROWIRE
compatible. This interface offers several flexible modes of
operation. These include internal/external serial clock,
2-or3-wireI/O,singlecycleconversionandautostart.The
following sections describe each of these serial interface
timing modes in detail. In all these cases, the converter
can use the internal oscillator (FO = LOW) or an external
oscillator connected to the FO pin. Refer to Table 4 for a
summary.
When CS (Pin 11) is HIGH, the SDO driver is switched to
a high impedance state. This allows sharing the serial
interface with other devices. If CS is LOW during the
convert or sleep state, SDO will output EOC. If CS is LOW
duringtheconversionphase, theEOCbitappearsHIGHon
the SDO pin. Once the conversion is complete, EOC goes
LOW. The device remains in the sleep state until the first
rising edge of SCK occurs while CS = LOW.
External Serial Clock, Single Cycle Operation
(SPI/MICROWIRE Compatible)
This timing mode uses an external serial clock to shift out
the conversion result and a CS signal to monitor and
control the state of the conversion cycle, see Figure 6.
Chip Select Input (CS)
The active LOW chip select, CS (Pin 11), is used to test the
conversionstatusandtoenablethedataoutputtransferas
described in the previous sections.
Table 4. LTC2413 Interface Timing Modes
Configuration
SCK Source Conversion Cycle Control
Data Output Control
CS and SCK
SCK
Connection and Waveforms
Figures 6, 7
External SCK, Single Cycle Conversion
External SCK, 2-Wire I/O
External
External
Internal
Internal
Internal
CS and SCK
SCK
Figure 8
Internal SCK, Single Cycle Conversion
Internal SCK, 2-Wire I/O, Continuous Conversion
Internal SCK, Autostart Conversion
CS ↓
CS ↓
Figures 9, 10
Figure 11
Continuous
Internal
C
Internal
Figure 12
EXT
sn2413 2413fs
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The serial clock mode is selected on the falling edge of CS.
Toselecttheexternalserialclockmode,theserialclockpin
(SCK) must be LOW during each CS falling edge.
As described above, CS may be pulled LOW at any time in
order to monitor the conversion status.
Typically, CS remains LOW during the data output state.
However, the data output state may be aborted by pulling
CS HIGH anytime between the first rising edge and the
32nd falling edge of SCK, see Figure 7. On the rising edge
of CS, the device aborts the data output state and imme-
diately initiates a new conversion. This is useful for sys-
tems not requiring all 32 bits of output data, aborting an
invalid conversion cycle or synchronizing the start of a
conversion.
The serial data output pin (SDO) is Hi-Z as long as CS is
HIGH. At any time during the conversion cycle, CS may be
pulled LOW in order to monitor the state of the converter.
While CS is pulled LOW, EOC is output to the SDO pin.
EOC = 1 while a conversion is in progress and EOC = 0 if
the device is in the sleep state. Independent of CS, the
deviceautomaticallyentersthelowpowersleepstateonce
the conversion is complete.
When the device is in the sleep state (EOC = 0), its
conversion result is held in an internal static shift regis-
ter. The device remains in the sleep state until the first
risingedgeofSCKisseenwhileCSisLOW.Dataisshifted
out the SDO pin on each falling edge of SCK. This enables
external circuitry to latch the output on the rising edge of
SCK. EOC can be latched on the first rising edge of SCK
and the last bit of the conversion result can be latched on
the 32nd rising edge of SCK. On the 32nd falling edge of
SCK, thedevicebeginsanewconversion. SDOgoesHIGH
(EOC = 1) indicating a conversion is in progress.
External Serial Clock, 2-Wire I/O
This timing mode utilizes a 2-wire serial I/O interface. The
conversion result is shifted out of the device by an exter-
nally generated serial clock (SCK) signal, see Figure 8. CS
may be permanently tied to ground, simplifying the user
interface or isolation barrier.
The external serial clock mode is selected at the end of the
power-on reset (POR) cycle. The POR cycle is concluded
approximately 0.5ms after VCC exceeds 2.2V. The level
applied to SCK at this time determines if SCK is internal or
external. SCK must be driven LOW prior to the end of POR
in order to enter the external serial clock timing mode.
At the conclusion of the data cycle, CS may remain LOW
and EOC monitored as an end-of-conversion interrupt.
Alternatively, CS may be driven HIGH setting SDO to Hi-Z.
2.7V TO 5.5V
1µF
= EXTERNAL OSCILLATOR
2
14
13
V
F
O
CC
= INTERNAL OSC/SIMULTANEOUS 50Hz/60Hz REJECTION
LTC2413
3
4
+
–
REFERENCE
VOLTAGE
REF
REF
SCK
0.1V TO V
CC
3-WIRE
SPI INTERFACE
5
6
12
11
+
ANALOG INPUT RANGE
–0.5V TO 0.5V
IN
SDO
CS
REF
REF
–
IN
1, 7, 8, 9, 10, 15, 16
GND
CS
TEST EOC
TEST EOC
TEST EOC
BIT 31
EOC
BIT 30
BIT 29
SIG
BIT 28
MSB
BIT 27
BIT 26
BIT 5
LSB
BIT 0
SDO
SUB LSB
Hi-Z
Hi-Z
Hi-Z
SCK
(EXTERNAL)
CONVERSION
SLEEP
DATA OUTPUT
CONVERSION
2413 F06
Figure 6. External Serial Clock, Single Cycle Operation
sn2413 2413fs
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LTC2413
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2.7V TO 5.5V
1µF
= EXTERNAL OSCILLATOR
2
14
13
V
F
O
CC
LTC2413
= INTERNAL OSC/SIMULTANEOUS 50Hz/60Hz REJECTION
3
+
REFERENCE
VOLTAGE
0.1V TO V
REF
REF
SCK
4
–
CC
3-WIRE
SPI INTERFACE
5
6
12
11
+
ANALOG INPUT RANGE
–0.5V TO 0.5V
IN
SDO
CS
REF
REF
–
IN
1, 7, 8, 9, 10, 15, 16
GND
CS
TEST EOC
TEST EOC
TEST EOC
BIT 0
EOC
BIT 31
EOC
BIT 30
BIT 29
SIG
BIT 28
MSB
BIT 27
BIT 9
BIT 8
SDO
Hi-Z
Hi-Z
Hi-Z
Hi-Z
SCK
(EXTERNAL)
SLEEP
CONVERSION
DATA OUTPUT
SLEEP
DATA OUTPUT
CONVERSION
2413 F07
Figure 7. External Serial Clock, Reduced Data Output Length
Since CS is tied LOW, the end-of-conversion (EOC) can be
continuously monitored at the SDO pin during the convert
and sleep states. EOC may be used as an interrupt to an
external controller indicating the conversion result is
ready. EOC = 1 while the conversion is in progress and
EOC = 0 once the conversion enters the low power sleep
state. On the falling edge of EOC, the conversion result is
loaded into an internal static shift register. The device
remains in the sleep state until the first rising edge of SCK.
Data is shifted out the SDO pin on each falling edge of SCK
enabling external circuitry to latch data on the rising edge
of SCK. EOC can be latched on the first rising edge of SCK.
Onthe32ndfallingedgeofSCK,SDOgoesHIGH(EOC = 1)
indicating a new conversion has begun.
enter the internal serial clock mode if SCK is driven LOW
on the falling edge of CS. An internal weak pull-up resistor
is active on the SCK pin during the falling edge of CS;
therefore, the internal serial clock timing mode is auto-
matically selected if SCK is not externally driven.
The serial data output pin (SDO) is Hi-Z as long as CS is
HIGH. At any time during the conversion cycle, CS may be
pulled LOW in order to monitor the state of the converter.
Once CS is pulled LOW, SCK goes LOW and EOC is output
to the SDO pin. EOC = 1 while a conversion is in progress
and EOC = 0 if the device is in the sleep state.
WhentestingEOC,iftheconversioniscomplete(EOC=0),
thedevicewillexitthesleepstateandenterthedataoutput
state if CS remains LOW. In order to prevent the device
from exiting the low power sleep state, CS must be pulled
HIGH before the first rising edge of SCK. In the internal
SCK timing mode, SCK goes HIGH and the device begins
outputting data at time tEOCtest after the falling edge of CS
(if EOC = 0) or tEOCtest after EOC goes LOW (if CS is LOW
duringthefallingedgeofEOC).ThevalueoftEOCtest is26µs
ifthedeviceisusingitsinternaloscillator(F0 =logicLOW).
Internal Serial Clock, Single Cycle Operation
This timing mode uses an internal serial clock to shift out
the conversion result and a CS signal to monitor and
control the state of the conversion cycle, see Figure 9.
In order to select the internal serial clock timing mode, the
serial clock pin (SCK) must be floating (Hi-Z) or pulled
HIGH prior to the falling edge of CS. The device will not
If FO is driven by an external oscillator of frequency fEOSC
,
sn2413 2413fs
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LTC2413
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2.7V TO 5.5V
1µF
= EXTERNAL OSCILLATOR
= INTERNAL OSC/SIMULTANEOUS 50Hz/60Hz REJECTION
2
14
13
V
F
O
CC
LTC2413
3
+
–
REFERENCE
VOLTAGE
0.1V TO V
REF
REF
SCK
4
CC
2-WIRE I/O
5
6
12
11
+
ANALOG INPUT RANGE
–0.5V TO 0.5V
IN
SDO
CS
REF REF
–
IN
1, 7, 8, 9, 10, 15, 16
GND
CS
BIT 31
EOC
BIT 30
BIT 29
SIG
BIT 28
MSB
BIT 27
BIT 26
BIT 5
LSB
BIT 0
SDO
24
SCK
(EXTERNAL)
CONVERSION
SLEEP
DATA OUTPUT
CONVERSION
2413 F08
Figure 8. External Serial Clock, CS = 0 Operation
2.7V TO 5.5V
V
CC
1µF
= EXTERNAL OSCILLATOR
= INTERNAL OSC/SIMULTANEOUS
50Hz/60Hz REJECTION
2
14
13
V
F
O
CC
10k
LTC2413
3
4
+
–
REFERENCE
VOLTAGE
REF
REF
SCK
0.1V TO V
CC
3-WIRE
SPI INTERFACE
5
6
12
11
+
ANALOG INPUT RANGE
–0.5V TO 0.5V
IN
SDO
CS
REF
REF
–
IN
1, 7, 8, 9, 10, 15, 16
GND
<t
EOCtest
CS
TEST EOC
TEST EOC
BIT 31
EOC
BIT 30
BIT 29
SIG
BIT 28
MSB
BIT 27
BIT 26
BIT 5
LSB
BIT 0
SDO
24
Hi-Z
Hi-Z
Hi-Z
Hi-Z
SCK
(INTERNAL)
CONVERSION
SLEEP
DATA OUTPUT
CONVERSION
2413 F09
Figure 9. Internal Serial Clock, Single Cycle Operation
sn2413 2413fs
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then tEOCtest is 3.6/fEOSC. If CS is pulled HIGH before time
new conversion. This is useful for systems not requiring
all 32 bits of output data, aborting an invalid conversion
cycle, or synchronizing the start of a conversion. If CS is
pulled HIGH while the converter is driving SCK LOW, the
internal pull-up is not available to restore SCK to a logic
HIGH state. This will cause the device to exit the internal
serial clock mode on the next falling edge of CS. This can
be avoided by adding an external 10k pull-up resistor to
theSCKpinorbyneverpullingCSHIGHwhenSCKisLOW.
t
EOCtest, the device remains in the sleep state. The conver-
sion result is held in the internal static shift register.
If CS remains LOW longer than tEOCtest, the first rising
edge of SCK will occur and the conversion result is serially
shiftedoutoftheSDOpin. Thedataoutputcyclebeginson
this first rising edge of SCK and concludes after the 32nd
rising edge. Data is shifted out the SDO pin on each falling
edgeofSCK.Theinternallygeneratedserialclockisoutput
to the SCK pin. This signal may be used to shift the
conversion result into external circuitry. EOC can be
latchedonthefirstrisingedgeofSCKandthelastbitofthe
conversionresultonthe32ndrisingedgeofSCK. Afterthe
32nd rising edge, SDO goes HIGH (EOC = 1), SCK stays
HIGH and a new conversion starts.
Whenever SCK is LOW, the LTC2413’s internal pull-up at
pin SCK is disabled. Normally, SCK is not externally driven
if the device is in the internal SCK timing mode. However,
certainapplicationsmayrequireanexternaldriveronSCK.
If this driver goes Hi-Z after outputting a LOW signal, the
LTC2413’s internal pull-up remains disabled. Hence, SCK
remains LOW. On the next falling edge of CS, the device is
switched to the external SCK timing mode. By adding an
external 10k pull-up resistor to SCK, this pin goes HIGH
once the external driver goes Hi-Z. On the next CS falling
edge, the device will remain in the internal SCK timing
mode.
Typically, CS remains LOW during the data output state.
However, the data output state may be aborted by pulling
CS HIGH anytime between the first and 32nd rising edge
of SCK, see Figure 10. On the rising edge of CS, the device
aborts the data output state and immediately initiates a
2.7V TO 5.5V
V
CC
1µF
= EXTERNAL OSCILLATOR
= INTERNAL OSC/SIMULTANEOUS
50Hz/60Hz REJECTION
2
14
13
V
F
O
CC
LTC2413
10k
3
+
REFERENCE
REF
REF
SCK
VOLTAGE
4
–
0.1V TO V
CC
3-WIRE
SPI INTERFACE
5
6
12
11
+
ANALOG INPUT RANGE
–0.5V TO 0.5V
IN
SDO
CS
REF REF
–
IN
1, 7, 8, 9, 10, 15, 16
<t
EOCtest
GND
>t
EOCtest
CS
TEST EOC
TEST EOC
TEST EOC
BIT 0
EOC
BIT 31
EOC
BIT 30
BIT 29
SIG
BIT 28
MSB
BIT 27
BIT 26
BIT 8
SDO
Hi-Z
Hi-Z
Hi-Z
Hi-Z
Hi-Z
SCK
(INTERNAL)
SLEEP
CONVERSION
DATA OUTPUT
SLEEP
DATA OUTPUT
CONVERSION
2413 F10
Figure 10. Internal Serial Clock, Reduced Data Output Length
sn2413 2413fs
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A similar situation may occur during the sleep state when
CS is pulsed HIGH-LOW-HIGH in order to test the conver-
sionstatus.Ifthedeviceisinthesleepstate(EOC=0),SCK
will go LOW. Once CS goes HIGH (within the time period
defined above as tEOCtest), the internal pull-up is activated.
For a heavy capacitive load on the SCK pin, the internal
pull-up may not be adequate to return SCK to a HIGH level
before CS goes low again. This is not a concern under
normal conditions where CS remains LOW after detecting
EOC = 0. This situation is easily overcome by adding an
external 10k pull-up resistor to the SCK pin.
weak pull-up is active during the POR cycle; therefore, the
internal serial clock timing mode is automatically selected
if SCK is not externally driven LOW (if SCK is loaded such
that the internal pull-up cannot pull the pin HIGH, the
external SCK mode will be selected).
During the conversion, the SCK and the serial data output
pin (SDO) are HIGH (EOC = 1). Once the conversion is
complete, SCK and SDO go LOW (EOC = 0) indicating the
conversion has finished and the device has entered the
low power sleep state. The part remains in the sleep state
a minimum amount of time (1/2 the internal SCK period)
thenimmediatelybeginsoutputtingdata.Thedataoutput
cyclebeginsonthefirstrisingedgeofSCKandendsafter
the 32nd rising edge. Data is shifted out the SDO pin on
each falling edge of SCK. The internally generated serial
clock is output to the SCK pin. This signal may be used
to shift the conversion result into external circuitry. EOC
can be latched on the first rising edge of SCK and the last
bit of the conversion result can be latched on the 32nd
rising edge of SCK. After the 32nd rising edge, SDO goes
HIGH(EOC=1)indicatinganewconversionisinprogress.
SCK remains HIGH during the conversion.
Internal Serial Clock, 2-Wire I/O,
Continuous Conversion
This timing mode uses a 2-wire, all output (SCK and SDO)
interface. The conversion result is shifted out of the device
by an internally generated serial clock (SCK) signal, see
Figure 11. CS may be permanently tied to ground, simpli-
fying the user interface or isolation barrier.
The internal serial clock mode is selected at the end of the
power-on reset (POR) cycle. The POR cycle is concluded
approximately 0.5ms after VCC exceeds 2.2V. An internal
2.7V TO 5.5V
1µF
= EXTERNAL OSCILLATOR
2
14
13
V
F
O
CC
LTC2413
= INTERNAL OSC/SIMULTANEOUS 50Hz/60Hz REJECTION
3
+
REFERENCE
REF
REF
SCK
VOLTAGE
4
–
0.1V TO V
CC
2-WIRE I/O
5
6
12
11
+
ANALOG INPUT RANGE
IN
SDO
CS
–0.5V
TO 0.5V
REF
REF
–
IN
1, 7, 8, 9, 10, 15, 16
GND
CS
BIT 31
EOC
BIT 30
BIT 29
SIG
BIT 28
MSB
BIT 27
BIT 26
BIT 5
LSB
BIT 0
SDO
24
SCK
(INTERNAL)
CONVERSION
DATA OUTPUT
CONVERSION
2413 F11
SLEEP
Figure 11. Internal Serial Clock, CS = 0 Continuous Operation
sn2413 2413fs
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Internal Serial Clock, Autostart Conversion
used to shift the conversion result into external circuitry.
After the 32nd rising edge, CS is pulled HIGH and a new
conversion is immediately started. This is useful in appli-
cations requiring periodic monitoring and ultralow power.
Figure 15 shows the average supply current as a function
of capacitance on CS.
This timing mode is identical to the internal serial clock,
2-wire I/O described above with one additional feature.
Instead of grounding CS, an external timing capacitor is
tied to CS.
While the conversion is in progress, the CS pin is held
HIGH by an internal weak pull-up. Once the conversion is
complete, the device enters the low power sleep state and
an internal 25nA current source begins discharging the
capacitor tied to CS, see Figure 12. The time the converter
spends in the sleep state is determined by the value of the
external timing capacitor, see Figures 13 and 14. Once the
voltageatCSfallsbelowaninternalthreshold(≈1.4V), the
device automatically begins outputting data. The data
output cycle begins on the first rising edge of SCK and
ends on the 32nd rising edge. Data is shifted out the SDO
pin on each falling edge of SCK. The internally generated
serial clock is output to the SCK pin. This signal may be
It should be noticed that the external capacitor discharge
current is kept very small in order to decrease the con-
verter power dissipation in the sleep state. In the autostart
mode, the analog voltage on the CS pin cannot be ob-
served without disturbing the converter operation using a
regular oscilloscope probe. When using this configura-
tion, it is important to minimize the external leakage
current at the CS pin by using a low leakage external
capacitor and properly cleaning the PCB surface.
The internal serial clock mode is selected every time the
voltage on the CS pin crosses an internal threshold volt-
age. An internal weak pull-up at the SCK pin is active while
2.7V TO 5.5V
1µF
= EXTERNAL OSCILLATOR
2
14
13
V
F
O
CC
= INTERNAL OSC/SIMULTANEOUS 50Hz/60Hz REJECTION
LTC2413
3
4
+
REFERENCE
VOLTAGE
REF
REF
SCK
–
0.1V TO V
CC
2-WIRE I/O
5
6
12
11
+
ANALOG INPUT RANGE
IN
SDO
CS
–0.5V
TO 0.5V
REF
REF
–
IN
1, 7, 8, 9, 10, 15, 16
GND
C
EXT
V
CC
CS
GND
BIT 31
EOC
BIT 30
BIT 29
SIG
BIT 0
SDO
Hi-Z
Hi-Z
SCK
(INTERNAL)
CONVERSION
DATA OUTPUT
CONVERSION
SLEEP
2413 F12
Figure 12. Internal Serial Clock, Autostart Operation
sn2413 2413fs
22
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7
6
5
4
3
2
CS is discharging; therefore, the internal serial clock
timing mode is automatically selected if SCK is floating. It
is important to ensure there are no external drivers pulling
SCK LOW while CS is discharging.
PRESERVING THE CONVERTER ACCURACY
The LTC2413 is designed to reduce as much as possible
the conversion result sensitivity to device decoupling,
PCB layout, antialiasing circuits, line frequency perturba-
tions and so on. Nevertheless, in order to preserve the
extreme accuracy capability of this part, some simple
precautions are desirable.
V
= 5V
CC
1
0
V
= 3V
CC
10
100
100000
1
1000
10000
CAPACITANCE ON CS (pF)
2413 F13
Figure 13. CS Capacitance vs tSAMPLE
Digital Signal Levels
8
7
6
The LTC2413’s digital interface is easy to use. Its digital
inputs(FO,CSandSCKinExternalSCKmodeofoperation)
accept standard TTL/CMOS logic levels and the internal
hysteresis receivers can tolerate edge rates as slow as
100µs.However,someconsiderationsarerequiredtotake
advantage of the exceptional accuracy and low supply
current of this converter.
V
= 5V
CC
5
V
= 3V
CC
4
3
2
1
0
The digital output signals (SDO and SCK in Internal SCK
mode of operation) are less of a concern because they are
not generally active during the conversion state.
10
100
10000
100000
0
1000
CAPACITANCE ON CS (pF)
While a digital input signal is in the range 0.5V to
(VCC – 0.5V), the CMOS input receiver draws additional
current from the power supply. It should be noted that,
when any one of the digital input signals (FO, CS and SCK
inExternalSCKmodeofoperation)iswithinthisrange,the
LTC2413 power supply current may increase even if the
signal in question is at a valid logic level. For micropower
operation, it is recommended to drive all digital input
2413 F14
Figure 14. CS Capacitance vs Output Rate
300
250
V
V
= 5V
= 3V
CC
CC
200
150
signals to full CMOS levels [VIL < 0.4V and VIH
(VCC – 0.4V)].
>
100
50
0
During the conversion period, the undershoot and/or
overshootofafastdigitalsignalconnectedtotheLTC2413
pins may severely disturb the analog to digital conversion
process.Undershootandovershootcanoccurbecauseof
the impedance mismatch at the converter pin when the
transition time of an external control signal is less than
twice the propagation delay from the driver to LTC2413.
Forreference,onaregularFR-4board,signalpropagation
sn2413 2413fs
1
10
100
1000
10000 100000
CAPACITANCE ON CS (pF)
2413 F15
Figure 15. CS Capacitance vs Supply Current
23
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velocity is approximately 183ps/inch for internal traces
and 170ps/inch for surface traces. Thus, a driver gener-
ating a control signal with a minimum transition time of
1ns must be connected to the converter pin through a
trace shorter than 2.5 inches. This problem becomes
particularly difficult when shared control lines are used
and multiple reflections may occur. The solution is to
carefully terminate all transmission lines close to their
characteristic impedance.
ence. In this situation, the user must reduce to a minimum
the loop area for the FO signal as well as the loop area for
the differential input and reference connections.
Driving the Input and Reference
The input and reference pins of the LTC2413 converter are
directly connected to a network of sampling capacitors.
Depending upon the relation between the differential input
voltage and the differential reference voltage, these ca-
pacitorsareswitchingbetweenthesefourpinstransfering
small amounts of charge in the process. A simplified
equivalent circuit is shown in Figure 16.
Parallel termination near the LTC2413 pin will eliminate
thisproblembutwillincreasethedriverpowerdissipation.
A series resistor between 27Ω and 56Ω placed near the
driver or near the LTC2413 pin will also eliminate this
problem without additional power dissipation. The actual
resistor value depends upon the trace impedance and
connection topology.
For a simple approximation, the source impedance RS
driving an analog input pin (IN+, IN–, REF+ or REF–) can be
considered to form, together with RSW and CEQ (see
Figure 16), a first order passive network with a time
constant τ = (RS + RSW) • CEQ. The converter is able to
sample the input signal with better than 1ppm accuracy if
the sampling period is at least 14 times greater than the
input circuit time constant τ. The sampling process on the
four input analog pins is quasi-independent so each time
constant should be considered by itself and, under worst-
case circumstances, the errors may add.
An alternate solution is to reduce the edge rate of the
control signals. It should be noted that using very slow
edges will increase the converter power supply current
during the transition time. The multiple ground pins used
in this package configuration, as well as the differential
input and reference architecture, reduce substantially the
converter’s sensitivity to ground currents.
When using the internal oscillator (FO = LOW), the
LTC2413’sfront-endswitched-capacitornetworkisclocked
at 69900Hz corresponding to a 14.3µs sampling period.
Thus, for settling errors of less than 1ppm, the driving
source impedance should be chosen such that
τ ≤ 14.3µs/14 = 1.02µs. When an external oscillator of
frequency fEOSC is used, the sampling period is 2/fEOSC
Particular attention must be given to the connection of the
FO signal when the LTC2413 is used with an external
conversion clock. This clock is active during the conver-
sion time and the normal mode rejection provided by the
internal digital filter is not very high at this frequency. A
normal mode signal of this frequency at the converter
reference terminals may result in DC gain and INL errors.
A normal mode signal of this frequency at the converter
input terminals may result in a DC offset error. Such
perturbations may occur due to asymmetric capacitive
coupling between the FO signal trace and the converter
input and/or reference connection traces. An immediate
solution is to maintain maximum possible separation
between the FO signal trace and the input/reference sig-
nals. When the FO signal is parallel terminated near the
converter, substantial AC current is flowing in the loop
formedbytheFO connectiontrace, theterminationandthe
ground return path. Thus, perturbation signals may be
inductively coupled into the converter input and/or refer-
and, for a settling error of less than 1ppm, τ ≤ 0.14/fEOSC
.
Input Current
If complete settling occurs on the input, conversion re-
sults will be unaffected by the dynamic input current. An
incomplete settling of the input signal sampling process
may result in gain and offset errors, but it will not degrade
theINLperformanceoftheconverter. Figure16showsthe
mathematical expressions for the average bias currents
flowing through the IN+ and IN– pins as a result of the
sampling charge transfers when integrated over a sub-
stantial time period (longer than 64 internal clock cycles).
sn2413 2413fs
24
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V
CC
I
+
+
REF
R
R
(TYP)
SW
SW
I
I
LEAK
LEAK
V
IN + VINCM − VREFCM
I IN+
=
=
20k
(
)
)
AVG
AVG
V
0.5• REQ
−VIN + VINCM − VREFCM
0.5• REQ
REF
I IN−
(
V
CC
V2
I
+
IN
1.5• VREF − VINCM + VREFCM
IN
I REF+
=
−
(TYP)
20k
I
I
(
)
LEAK
LEAK
AVG
0.5• REQ
V
REF • REQ
V
+
IN
V2
−1.5• VREF − VINCM + VREFCM
0.5• REQ
C
IN
I REF−
=
+
EQ
(
)
18pF
AVG
V
REF • REQ
(TYP)
V
where:
CC
I
–
–
IN
IN
VREF = REF+ −REF−
R
R
(TYP)
SW
I
I
LEAK
LEAK
20k
REF+ + REF−
V
VREFCM
=
2
V
IN = IN+ −IN−
V
CC
I
–
–
REF
IN+ − IN−
(TYP)
20k
SW
V
INCM
=
I
I
LEAK
LEAK
2
2413 F16
V
REF
REQ = 3.97MΩ INTERNAL OSCILLATOR
REQ = 0.555• 1012 / fEOSC EXTERNAL OSCILLATOR
(
)
SWITCHING FREQUENCY
f
f
= 69900Hz INTERNAL OSCILLATOR
SW
SW
= 0.5 • f
EXTERNAL OSCILLATOR
EOSC
Figure 16. LTC2413 Equivalent Analog Input Circuit
R
SOURCE
The effect of this input dynamic current can be analyzed
using the test circuit of Figure 17. The CPAR capacitor
includes the LTC2413 pin capacitance (5pF typical) plus
thecapacitanceofthetestfixtureusedtoobtaintheresults
shown in Figures 18 and 19. A careful implementation can
bring the total input capacitance (CIN + CPAR) closer to 5pF
thus achieving better performance than the one predicted
by Figures 18 and 19. For simplicity, two distinct situa-
tions can be considered.
+
IN
C
C
PAR
V
+ 0.5V
C
C
INCM
INCM
IN
IN
IN
20pF
LTC2413
R
SOURCE
–
IN
2413 F17
PAR
20pF
V
– 0.5V
IN
Figure 17. An RC Network at IN+ and IN–
50
0
C
= 0.01µF
IN
V
= 5V
CC
+
REF = 5V
C
= 0.001µF
IN
C
–
REF = GND
40
30
20
10
0
–10
–20
–30
–40
–50
+
–
= 100pF
IN
IN = GND
IN = 2.5V
C
= 0pF
IN
F
= GND
= 25°C
O
A
T
V
= 5V
CC
+
–
REF = 5V
C
= 0.01µF
REF = GND
IN
+
–
IN = 5V
C
= 0.001µF
IN
C
IN = 2.5V
F
= GND
O
= 100pF
IN
C
T
= 25°C
A
= 0pF
IN
1.E+00 1.E+01 1.E+02 1.E+03 1.E+04 1.E+05
(Ω)
1.E+00 1.E+01 1.E+02 1.E+03 1.E+04 1.E+05
(Ω)
R
R
SOURCE
SOURCE
2413 F18
2413 F19
Figure 18. +FS Error vs RSOURCE at IN+ or IN– (Small CIN)
Figure 19. –FS Error vs RSOURCE at IN+ or IN– (Small CIN)
sn2413 2413fs
25
LTC2413
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For relatively small values of input capacitance (CIN
<
converter average input current will not degrade the INL
performance,indirectdistortionmayresultfromthemodu-
lation of the offset error by the common mode component
of the input signal. Thus, when using large CIN capacitor
values, itisadvisabletocarefullymatchthesourceimped-
ance seen by the IN+ and IN– pins. When internal oscillator
is used (FO = LOW), every 1Ω mismatch in source imped-
ance transforms a full-scale common mode input signal
into a differential mode input signal of 0.25ppm. When FO
0.01µF), the voltage on the sampling capacitor settles
almost completely and relatively large values for the
source impedance result in only small errors. Such values
for CIN will deteriorate the converter offset and gain
performancewithoutsignificantbenefitsofsignalfiltering
and the user is advised to avoid them. Nevertheless, when
small values of CIN are unavoidably present as parasitics
of input multiplexers, wires, connectors or sensors, the
LTC2413 can maintain its exceptional accuracy while
operatingwithrelativelargevaluesofsourceresistanceas
shown in Figures 18 and 19. These measured results may
be slightly different from the first order approximation
suggested earlier because they include the effect of the
actual second order input network together with the non-
linearsettlingprocessoftheinputamplifiers.ForsmallCIN
values, the settling on IN+ and IN– occurs almost indepen-
dently and there is little benefit in trying to match the
source impedance for the two pins.
is driven by an external oscillator with a frequency fEOSC
,
every 1Ω mismatch in source impedance transforms a
full-scale common mode input signal into a differential
mode input signal of 1.78 • 10–6 • fEOSCppm. Figure 22
shows the typical offset error due to input common mode
voltage for various values of source resistance imbalance
between the IN+ and IN– pins when large CIN values are
used.
If possible, it is desirable to operate with the input signal
common mode voltage very close to the reference signal
common mode voltage as is the case in the ratiometric
measurement of a symmetric bridge. This configuration
eliminates the offset error caused by mismatched source
impedances.
Larger values of input capacitors (CIN > 0.01µF) may be
required in certain configurations for antialiasing or gen-
eral input signal filtering. Such capacitors will average the
input sampling charge and the external source resistance
will see a quasi constant input differential impedance.
When internal oscillator is used (FO= LOW), the typical
differential input resistance is 2MΩ which will generate a
gain error of approximately 0.25ppm for each ohm of
source resistance driving IN+ or IN–. When FO is driven by
an external oscillator with a frequency fEOSC (external
conversion clock operation), the typical differential input
resistance is 0.28 • 1012/fEOSCΩ and each ohm of
source resistance driving IN+ or IN– will result in
1.78 • 10–6 • fEOSCppm gain error. The effect of the source
resistance on the two input pins is additive with respect to
thisgainerror.Thetypical+FSand–FSerrorsasafunction
of the sum of the source resistance seen by IN+ and IN– for
large values of CIN are shown in Figures 20 and 21.
Themagnitudeofthedynamicinputcurrentdependsupon
thesizeoftheverystableinternalsamplingcapacitorsand
upon the accuracy of the converter sampling clock. The
accuracy of the internal clock over the entire temperature
and power supply range is typical better than 0.5%. Such
a specification can also be easily achieved by an external
clock. When relatively stable resistors (50ppm/°C) are
used for the external source impedance seen by IN+ and
IN–, the expected drift of the dynamic current, offset and
gain errors will be insignificant (about 1% of their respec-
tive values over the entire temperature and voltage range).
Even for the most stringent applications a one-time cali-
bration operation may be sufficient.
In addition to the input sampling charge, the input ESD
protection diodes have a temperature dependent leakage
current. This current, nominally 1nA (±10nA max), results
inasmalloffsetshift. A100Ωsourceresistancewillcreate
a 0.1µV typical and 1µV maximum offset voltage.
In addition to this gain error, an offset error term may also
appear. The offset error is proportional with the mismatch
between the source impedance driving the two input pins
IN+ and IN– and with the difference between the input and
reference common mode voltages. While the input drive
circuit nonzero source impedance combined with the
sn2413 2413fs
26
LTC2413
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300
Reference Current
V
= 5V
CC
+
REF = 5V
–
C
= 1µF, 10µF
In a similar fashion, the LTC2413 samples the differential
reference pins REF+ and REF– transfering small amount of
charge to and from the external driving circuits, thus
produces a dynamic reference current. This current does
notchangetheconverteroffsetbutitmaydegradethegain
and INL performance. The effect of this current can be
analyzed in the same two distinct situations.
IN
REF = GND
240
180
120
60
+
–
IN = 3.75V
IN = 1.25V
F
= GND
= 25°C
O
A
T
C
IN
= 0.1µF
C
IN
= 0.01µF
Forrelativelysmallvaluesoftheexternalreferencecapaci-
tors(CREF <0.01µF),thevoltageonthesamplingcapacitor
settles almost completely and relatively large values for
the source impedance result in only small errors. Such
values for CREF will deteriorate the converter offset and
gainperformancewithoutsignificantbenefitsofreference
filtering and the user is advised to avoid them.
0
0
100 200 300 400 500 600 700 800 9001000
(Ω)
R
SOURCE
2413 F19
Figure 20. +FS Error vs RSOURCE at IN+ or IN– (Large CIN)
0
C
IN
= 0.01µF
–60
–120
–180
–240
–300
Larger values of reference capacitors (CREF > 0.01µF) may
be required as reference filters in certain configurations.
Suchcapacitorswillaveragethereferencesamplingcharge
and the external source resistance will see a quasi con-
stant reference differential impedance. When internal os-
cillator is used (FO = LOW), the typical differential input
resistance is 1.43MΩ which will generate a gain error of
approximately 0.35ppm for each ohm of source resis-
tance driving REF+ or REF–. When FO is driven by an
externaloscillatorwithafrequencyfEOSC (externalconver-
sion clock operation), the typical differential reference
resistance is 0.20 • 1012/fEOSCΩ and each ohm of source
resistance drving REF+ or REF– will result in
2.47 • 10–6 • fEOSCppm gain error. The effect of the source
resistance on the two reference pins is additive with
respect to this gain error. The typical +FS and –FS errors
for various combinations of source resistance seen by the
REF+ and REF– pins and external capacitance CREF con-
nected to these pins are shown in Figures 23, 24, 25
and 26.
C
IN
= 0.1µF
V
= 5V
CC
+
REF = 5V
–
REF = GND
+
–
IN = 1.25V
IN = 3.75V
C
IN
= 1µF, 10µF
F
= GND
= 25°C
O
A
T
0
100 200 300 400 500 600 700 800 9001000
(Ω)
R
SOURCE
2413 F21
Figure 21. –FS Error vs RSOURCE at IN+ or IN– (Large CIN)
120
V
= 5V
CC
+
100
80
REF = 5V
–
A
B
REF = GND
IN = IN = V
+
–
INCM
60
40
C
D
E
F
20
0
–20
–40
–60
–80
–100
–120
G
F
= GND
O
A
T
= 25°C
R
C
– = 500Ω
SOURCEIN
= 10µF
In addition to this gain error, the converter INL perfor-
mance is degraded by the reference source impedance.
Wheninternaloscillatorisused(FO =LOW), every100Ωof
source impedance driving REF+ or REF– translates into
about 1.2ppm additional INL error. When FO is driven by
an external oscillator with a frequency fEOSC, every 100Ω
of source resistance driving REF+ or REF– translates into
IN
0
0.5
1
1.5
2
2.5
3
3.5
4
4.5
5
V
INCM
(V)
A: ∆R = +400Ω
E: ∆R = –100Ω
IN
IN
IN
IN
IN
B: ∆R = +200Ω
F: ∆R = –200Ω
IN
C: ∆R = +100Ω
G: ∆R = –400Ω
IN
D: ∆R = 0Ω
2413 F22
Figure 22. Offset Error vs Common Mode Voltage
(VINCM = IN+ = IN–) and Input Source Resistance Imbalance
(∆RIN = RSOURCEIN+ – RSOURCEIN–) for Large CIN Values (CIN ≥ 1µF)
about 8.73 • 10–6 • fEOSCppm additional INL error.
sn2413 2413fs
27
LTC2413
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Figure 27 shows the typical INL error due to the source
resistance driving the REF+ or REF– pins when large CREF
values are used. The effect of the source resistance on the
tworeferencepinsisadditivewithrespecttothisINLerror.
In general, matching of source impedance for the REF+
and REF– pins does not help the gain or the INL error. The
user is thus advised to minimize the combined source
impedance driving the REF+ and REF– pins rather than to
try to match it.
0.5%. Such a specification can also be easily achieved by
an external clock. When relatively stable resistors
(50ppm/°C) are used for the external source impedance
seen by REF+ and REF–, the expected drift of the dynamic
current gain error will be insignificant (about 1% of its
valueovertheentiretemperatureandvoltagerange). Even
for the most stringent applications, a one-time calibration
operation may be sufficient.
Inadditiontothereferencesamplingcharge,thereference
pinsESDprotectiondiodeshaveatemperaturedependent
leakage current. This leakage current, nominally 1nA
(±10nA max), results in a small gain error. A 100Ω source
resistance will create a 0.05µV typical and 0.5µV maxi-
mum full-scale error.
The magnitude of the dynamic reference current depends
upon the size of the very stable internal sampling capaci-
tors and upon the accuracy of the converter sampling
clock. The accuracy of the internal clock over the entire
temperature and power supply range is typical better than
0
50
C
= 0.01µF
REF
V
= 5V
CC
+
REF = 5V
C
= 0.001µF
REF
–
REF = GND
–10
–20
–30
–40
–50
40
30
20
10
0
+
–
C
= 100pF
IN = 5V
REF
IN = 2.5V
C
= 0pF
REF
F
= GND
= 25°C
O
A
T
V
= 5V
CC
+
–
REF = 5V
C
= 0.01µF
REF = GND
REF
+
–
IN = GND
C
= 0.001µF
REF
IN = 2.5V
F
= GND
O
C
= 100pF
REF
T
= 25°C
A
C
= 0pF
REF
1.E+00 1.E+01 1.E+02 1.E+03 1.E+04 1.E+05
(Ω)
1.E+00 1.E+01 1.E+02 1.E+03 1.E+04 1.E+05
(Ω)
R
R
SOURCE
SOURCE
2413 F23
2413 F24
Figure 23. +FS Error vs RSOURCE at REF+ or REF– (Small CREF
)
Figure 24. –FS Error vs RSOURCE at REF+ or REF– (Small CREF
)
0
450
C
= 0.01µF
= 0.1µF
REF
V
= 5V
CC
+
REF = 5V
C
REF
= 1µF, 10µF
–
REF = GND
–90
–180
–270
–360
–450
360
270
180
90
+
–
IN = 1.25V
IN = 3.75V
F
= GND
= 25°C
O
A
C
REF
T
V
= 5V
CC
C
REF
= 0.1µF
+
REF = 5V
–
REF = GND
+
–
IN = 3.75V
IN = 1.25V
C
REF
= 0.01µF
C
= 1µF, 10µF
REF
F
= GND
= 25°C
O
A
T
0
0
100 200 300 400 500 600 700 800 9001000
(Ω)
0
100 200 300 400 500 600 700 800 9001000
(Ω)
R
R
SOURCE
SOURCE
2413 F25
2413 F26
Figure 25. +FS Error vs RSOURCE at REF+ or REF– (Large CREF
)
Figure 26. –FS Error vs RSOURCE at REF+ or REF– (Large CREF
)
sn2413 2413fs
28
LTC2413
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APPLICATIO S I FOR ATIO
15
12
9
R
= 1000Ω
SOURCE
R
= 500Ω
6
SOURCE
3
0
–3
–6
–9
–12
–15
R
= 100Ω
SOURCE
–0.5–0.4–0.3–0.2–0.1
0
0.1 0.2 0.3 0.4 0.5
V
/V
INDIF REFDIF
V
= 5V
F = GND
O
CC
REF+ = 5V
C
= 10µF
REF
REF– = GND
V
T = 25°C
A
+
–
= 0.5 • (IN + IN ) = 2.5V
2413 F27
INCM
Figure 27. INL vs Differential Input Voltage (VIN = IN+ – IN–)
and Reference Source Resistance (RSOURCE at REF+ and REF– for
Large CREF Values (CREF ≥ 1µF)
First, a change in fEOSC will result in a proportional change
in the internal notch position and in a reduction of the
converter differential mode rejection at the power-line
frequency. In many applications, the subsequent perfor-
mance degradation can be substantially reduced by rely-
ing upon the LTC2413’s exceptional common mode rejec-
tion and by carefully eliminating common mode to differ-
ential mode conversion sources in the input circuit. The
user should avoid single-ended input filters and should
maintain a very high degree of matching and symmetry in
the circuits driving the IN+ and IN– pins.
Output Data Rate
When using its internal oscillator, the LTC2413 can pro-
duceupto6.8readingspersecond. Theactualoutputdata
rate will depend upon the length of the sleep and data
output phases which are controlled by the user and which
can be made insignificantly short. When operated with an
external conversion clock (FO connected to an external
oscillator), the LTC2413 output data rate can be increased
asdesired. Thedurationoftheconversionphaseis20510/
fEOSC. If fEOSC = 139800Hz, the converter behaves as if the
internal oscillator is used with simultaneous 50Hz/60Hz
rejection. ThereisnosignificantdifferenceintheLTC2413
performance between these two operation modes.
Second, the increase in clock frequency will increase
proportionally the amount of sampling charge transferred
through the input and the reference pins. If large external
input and/or reference capacitors (CIN, CREF) are used, the
previous section provides formulae for evaluating the
effect of the source resistance upon the converter perfor-
mance for any value of fEOSC. If small external input and/
or reference capacitors (CIN, CREF) are used, the effect of
the external source resistance upon the LTC2413 typical
performance can be inferred from Figures 18, 19, 23 and
An increase in fEOSC over the nominal 139800Hz will
translate into a proportional increase in the maximum
output data rate. This substantial advantage is neverthe-
less accompanied by three potential effects, which must
be carefully considered.
24 in which the horizontal axis is scaled by 139800/fEOSC
.
sn2413 2413fs
29
LTC2413
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Third, an increase in the frequency of the external oscilla-
torabove460800Hz(amorethan3×increaseintheoutput
data rate) will start to decrease the effectiveness of the
internal autocalibration circuits. This will result in a pro-
gressive degradation in the converter accuracy and linear-
ity. Typical measured performance curves for output data
rates up to 100 readings per second are shown in Fig-
ures 28 through 35, inclusive. In order to obtain the
highest possible level of accuracy from this converter at
output data rates above 20 readings per second, the user
is advised to maximize the power supply voltage used and
to limit the maximum ambient operating temperature. In
certaincircumstances, areductionofthedifferentialrefer-
ence voltage may be beneficial.
500
V
= 5V
450
400
350
300
250
200
150
100
50
CC
+
REF = 5V
–
REF = GND
V
V
O
= 2.5V
INCM
= 0V
IN
= EXTERNAL OSCILLATOR
F
T
= 85°C
A
T
A
= 25°C
0
0
10 20 30 40 50 60 70 80 90 100
OUTPUT DATA RATE (READINGS/SEC)
2413 F28
Figure 28. Offset Error vs Output Data Rate and Temperature
7000
6000
5000
4000
3000
2000
1000
0
0
–1000
–2000
V
= 5V
CC
+
REF = 5V
–
T
= 85°C
REF = GND
A
+
–
IN = 3.75V
IN = 1.25V
T
A
= 25°C
F
O
= EXTERNAL OSCILLATOR
–3000
–4000
–5000
–6000
–7000
V
= 5V
CC
T
A
= 85°C
+
REF = 5V
–
REF = GND
+
–
IN = 1.25V
T
A
= 25°C
IN = 3.75V
F
= EXTERNAL OSCILLATOR
O
0
10 20 30 40 50 60 70 80 90 100
OUTPUT DATA RATE (READINGS/SEC)
0
10 20 30 40 50 60 70 80 90 100
OUTPUT DATA RATE (READINGS/SEC)
2413 F29
2413 F30
Figure 29. +FS Error vs Output Data Rate and Temperature
Figure 30. –FS Error vs Output Data Rate and Temperature
sn2413 2413fs
30
LTC2413
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24
23
22
22
20
18
16
14
12
10
8
RESOLUTION = LOG (V /INL )
MAX
2
REF
T
= 25°C
A
21
20
19
18
17
16
15
14
13
12
T
= 85°C
T = 25°C
A
A
T
= 85°C
A
V
= 5V
CC
+
V
= 5V
REF = 5V
CC
+
–
REF = 5V
REF = GND
–
REF = GND
V
V
F
= 2.5V
INCM
V
= 2.5V
= 0V
INCM
IN
–2.5V < V < 2.5V
= EXTERNAL OSCILLATOR
RESOLUTION = LOG (V /NOISE )
RMS
IN
O
F
O
= EXTERNAL OSCILLATOR
2
REF
0
10 20 30 40 50 60 70 80 90 100
OUTPUT DATA RATE (READINGS/SEC)
0
10 20 30 40 50 60 70 80 90 100
OUTPUT DATA RATE (READINGS/SEC)
2413 F31
2413 F32
Figure 32. Resolution (INLRMS ≤ 1LSB)
vs Output Data Rate and Temperature
Figure 31. Resolution (NoiseRMS ≤ 1LSB)
vs Output Data Rate and Temperature
250
24
23
V
= 5V
225
200
175
150
125
100
75
CC
V
= 5V
REF
+
REF = GND
22
21
20
19
18
17
16
15
14
13
12
V
V
= 2.5V
INCM
= 0V
V
= 2.5V
IN
REF
F
= EXTERNAL OSCILLATOR
= 25°C
O
A
T
V
= 5V
CC
–
REF = GND
V
= 5V
REF
V
V
F
= 2.5V
INCM
= 0V
IN
V
= 2.5V
REF
= EXTERNAL OSCILLATOR
= 25°C
50
O
T
A
25
RESOLUTION = LOG (V /NOISE )
RMS
2
REF
0
0
10 20 30 40 50 60 70 80 90 100
OUTPUT DATA RATE (READINGS/SEC)
0
10 20 30 40 50 60 70 80 90 100
OUTPUT DATA RATE (READINGS/SEC)
2413 F33
2413 F34
Figure 33. Offset Error vs Output
Data Rate and Reference Voltage
Figure 34. Resolution (NoiseRMS ≤ 1LSB) vs
Output Data Rate and Reference Voltage
22
RESOLUTION =
LOG (V /INL
)
20
18
16
14
12
10
8
2
REF
MAX
V
= 2.5V
V
= 5V
REF
REF
T
= 25°C
= 5V
A
CC
V
–
REF = GND
= 0.5 • REF
+
V
INCM
–0.5V • V
< V < 0.5 • V
REF
IN REF
F
= EXTERNAL OSCILLATOR
O
0
10 20 30 40 50 60 70 80 90 100
OUTPUT DATA RATE (READINGS/SEC)
2413 F35
Figure 35. Resolution (INLMAX ≤ 1LSB) vs Output Data Rate and Reference Voltage
sn2413 2413fs
31
LTC2413
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APPLICATIO S I FOR ATIO
Input Bandwidth
high gain, low bandwidth amplifier stage followed by a
high bandwidth unity-gain buffer.
The combined effect of the internal sinc4 digital filter and
of the analog and digital autocalibration circuits deter-
mines the LTC2413 input bandwidth. When the internal
oscillator is used (FO = LOW), the 3dB input bandwidth is
3.3Hz. If an external conversion clock generator of fre-
quency fEOSC is connected to the FO pin, the 3dB input
When external amplifiers are driving the LTC2413, the
ADCinputreferredsystemnoisecalculationcanbesimpli-
fied by Figure 37. The noise of an amplifier driving the
LTC2413 input pin can be modeled as a band limited white
noise source. Its bandwidth can be approximated by the
bandwidth of a single pole lowpass filter with a corner
frequency fi. The amplifier noise spectral density is ni.
From Figure 37, using fi as the x-axis selector, we can find
on the y-axis the noise equivalent bandwidth freqi of the
input driving amplifier. This bandwidth includes the band
limitingeffectsoftheADCinternalcalibrationandfiltering.
The noise of the driving amplifier referred to the converter
input and including all these effects can be calculated as
N = ni • √freqi. The total system noise (referred to the
LTC2413 input) can now be obtained by summing as
squarerootofsumofsquaresthethreeADCinputreferred
noise sources: the LTC2413 internal noise (800nV), the
noise of the IN+ driving amplifier and the noise of the IN–
driving amplifier.
bandwidth is 0.236 • 10–6 • fEOSC
.
Due to the complex filtering and calibration algorithms
utilized,theconverterinputbandwidthisnotmodeledvery
accurately by a first order filter with the pole located at the
3dB frequency. When the internal oscillator is used, the
shape of the LTC2413 input bandwidth is shown in
Figure 36. When an external oscillator of frequency fEOSC
is used, the shape of the LTC2413 input bandwidth can be
derived from Figure 36, in which the horizontal axis is
scaled by fEOSC/139800.
The conversion noise (800nVRMS typical for VREF = 5V)
can be modeled as a white noise source connected to a
noisefreeconverter.Thenoisespectraldensityis63nV/√Hz
for an infinite bandwidth source and 77nV/√Hz for a single
0.5MHz pole source. From these numbers, it is clear that
particular attention must be given to the design of external
amplification circuits. Such circuits face the simultaneous
requirements of very low bandwidth (just a few Hz) in
order to reduce the output referred noise and relatively
high bandwidth (at least 500kHz) necessary to drive the
input switched-capacitor network. A possible solution is a
If the FO pin is driven by an external oscillator of frequency
fEOSC, Figure37canstillbeusedfornoisecalculationifthe
x-axis is scaled by fEOSC/139800. For large values of the
ratio fEOSC/139800, the Figure 37 plot accuracy begins to
decrease, but in the same time the LTC2413 noise floor
rises and the noise contribution of the driving amplifiers
lose significance.
1000
100
0.0
–0.5
–1.0
–1.5
–2.0
–2.5
–3.0
–3.5
–4.0
–4.5
–5.0
–5.5
–6.0
F
= LOW
O
10
1
0.1
0.1
0
0.5
1
1.5
2
2.5
3
3.5
4
4.5
5
1
10 100 1k 10k 100k 1M
DIFFERENTIAL INPUT SIGNAL FREQUENCY (Hz)
INPUT NOISE SOURCE SINGLE POLE
EQUIVALENT BANDWIDTH (Hz)
2413 F37
2413 F36
Figure 36. Input Signal Bandwidth Using the Internal Oscillator
Figure 37. Input Referred Noise Equivalent Bandwidth
of an Input Connected White Noise Source
sn2413 2413fs
32
LTC2413
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Normal Mode Rejection and Antialiasing
the maximum output data rate. In the internal oscillator
mode, fS = 13980Hz. In the external oscillator mode, fS =
fEOSC/10.
One of the advantages delta-sigma ADCs offer over con-
ventional ADCs is on-chip digital filtering. Combined with
a large oversampling ratio, the LTC2413 significantly
simplifies antialiasing filter requirements.
The sinc4 digital filter provides greater than 120dB normal
mode rejection at all frequencies except DC and integer
multiples of the modulator sampling frequency (fS). The
LTC2413’s autocalibration circuits further simplify the
antialiasing requirements by additional normal mode sig-
nal filtering both in the analog and digital domain. Inde-
pendent of the operating mode, fS = 256 • fN = 2048 •
fOUTMAX where fN in the notch frequency and fOUTMAX is
The combined normal mode rejection performance is
showninFigure 38. Theregionsoflowrejectionoccurring
at integer multiples of fS have a very narrow bandwidth.
Magnified details of the normal mode rejection curves are
shown in Figure 39 (rejection near DC) and Figure 40
(rejection at fS = 256fN) where fN represents the notch
frequency. These curves have been derived for the exter-
nal oscillator mode but they can be used in all operating
modes by appropriately selecting the fN value.
0
–10
–20
–30
–40
–50
–60
–70
–80
–90
–100
–110
–120
F
F
= LOW OR
O
O
= EXTERNAL OSCILLATOR,
f
= 10 • f
EOSC
S
0
f
2f 3f 4f 5f 6f 7f 8f 9f 10f
S S S S S S S S S S
DIFFERENTIAL INPUT SIGNAL FREQUENCY (Hz)
2413 F38
Figure 38. Input Normal Mode Rejection
0
–10
–20
–30
–40
–50
–60
–70
–80
–90
–100
–110
–120
0
–10
–20
–30
–40
–50
–60
–70
–80
–90
–100
–110
–120
250f 252f 254f 256f 258f 260f 262f
N
0
f
2f
N
3f
4f
N
5f
6f
7f
8f
N
N
N
N
N
N
N
N
N
N
N
N
INPUT SIGNAL FREQUENCY (Hz)
INPUT SIGNAL FREQUENCY (Hz)
2413 F40
2413 F39
Figure 39. Input Normal Mode Rejection
Figure 40. Input Normal Mode Rejection
sn2413 2413fs
33
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The user can expect to achieve in practice this level of
performance using the internal oscillator, as it is demon-
strated by Figure 41. Typical measured values of the
normal mode rejection of the LTC2413 operating with the
internal oscillator are shown in Figure 41 superimposed
over the theoretical calculated curve.
Traditional high order delta-sigma modulators, while pro-
viding very good linearity and resolution, suffer from po-
tential instabilities at large input signal levels. The propri-
etaryarchitectureusedfortheLTC2413thirdordermodu-
lator resolves this problem and guarantees a predictable
stable behavior at input signal levels of up to 150% of full
scale. In many industrial applications, it is not uncommon
to have to measure microvolt level signals superimposed
over volt level perturbations and LTC2413 is eminently
suitedforsuchtasks.Whentheperturbationisdifferential,
the specification of interest is the normal mode rejection
for large input signal levels. With a reference voltage
As a result of these remarkable normal mode specifica-
tions, minimal (if any) antialias filtering is required in front
of the LTC2413. If passive RC components are placed in
front of the LTC2413, the input dynamic current should be
considered (see Input Current section). In cases where
large effective RC time constants are used, an external
buffer amplifier may be required to minimize the effects of
dynamic input current.
V
REF = 5V, the LTC2413 has a full-scale differential input
0
–20
–40
–60
–80
–100
–120
0
20
40
60
80
100
120
140
160
180
200
220
INPUT FREQUENCY (Hz)
2413 F41
Figure 41. Input Normal Mode Rejection vs Input
Frequency with Input Perturbation of 100% of Full Scale
sn2413 2413fs
34
LTC2413
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APPLICATIO S I FOR ATIO
range of 5V peak-to-peak. Figure 42 shows measurement
results for the LTC2413 normal mode rejection ratio with
a 7.5V peak-to-peak (150% of full scale) input signal su-
perimposed over the more traditional normal mode rejec-
tion ratio results obtained with a 5V peak-to-peak (full
scale) input signal. It is clear that the LTC2413 rejection
performance is maintained with no compromises in this
extreme situation. When operating with large input signal
levels, the user must observe that such signals do not
violate the device’s absolute maximum ratings.
limited to 5V. This gives only 10mV full scale, which can
beresolvedto1partin10000withoutaveraging.Formany
solid state sensors, this is still better than the sensor. For
example, averaging 64 samples however reduces the
noise level by a factor of eight, bringing the resolving
power to 1 part in 80000, comparable to better weighing
systems. Hysteresis and creep effects in the load cells are
typically much greater than this. Most applications that
require strain measurements to this level of accuracy are
measuring slowly changing phenomena, hence the time
required to average a large number of readings is usually
not an issue. For those systems that require accurate
measurement of a small incremental change on a signifi-
cant tare weight, the lack of history effects in the LTC2400
family is of great benefit.
BRIDGE APPLICATIONS
Typical strain gauge based bridges deliver only 2mV/Volt
of excitation. As the maximum reference voltage of the
LTC2413 is 5V, remote sensing of applied excitation
without additional circuitry requires that excitation be
0
–20
V
V
= 5V
= 7.5V
V
= 5V
IN(P-P)
CC
+
REF = 5V
REF = GND
IN(P-P)
–
(150% OF FULL SCALE)
V
= 2.5V
INCM
= 25°C
–40
T
A
–60
–80
–100
–120
0
20
40
60
80
100
120
140
160
180
200
220
INPUT FREQUENCY (Hz)
2413 F42
Figure 42. Measured Input Normal Mode Rejection vs Input
Frequency with Input Perturbation of 150% of Full Scale
sn2413 2413fs
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For those applications that cannot be fulfilled by the
LTC2413 alone, compensating for error in external ampli-
fication can be done effectively due to the “no latency”
feature of the LTC2413. No latency operation allows
samples of the amplifier offset and gain to be interleaved
withweighingmeasurements.Theuseofcorrelateddouble
sampling allows suppression of 1/f noise, offset and
thermocouple effects within the bridge. Correlated double
samplinginvolvesalternatingthepolarityofexcitationand
dealing with the reversal of input polarity mathematically.
Alternatively, bridge excitation can be increased to as
much as ±10V, if one of several precision attenuation
techniquesisusedtoproduceaprecisiondivideoperation
on the reference signal. Another option is the use of a
reference within the 5V input range of the LTC2413 and
developing excitation via fixed gain, or LTC1043 based
voltage multiplication, along with remote feedback in the
excitation amplifiers, as shown in Figures 48 and 50.
cells located at each load bearing point, the output of
which can be summed passively prior to the signal pro-
cessing circuitry, actively with amplification prior to the
ADC, or can be digitized via multiple ADC channels and
summed mathematically. The mathematical summation
oftheoutputofmultipleLTC2413’sprovidesthebenefitof
arootsquarereductioninnoise. Thelowpowerconsump-
tion of the LTC2413 makes it attractive for multidrop
communication schemes where the ADC is located within
the load-cell housing.
A direct connection to a load cell is perhaps best incorpo-
rated into the load-cell body, as minimizing the distance to
the sensor largely eliminates the need for protection
devices, RFI suppression and wiring. The LTC2413 exhib-
its extremely low temperature dependent drift. As a result,
exposure to external ambient temperature ranges does
not compromise performance. The incorporation of any
amplification considerably complicates thermal stability,
as input offset voltages and currents, temperature coeffi-
cient of gain settling resistors all become factors.
Figure 43 shows an example of a simple bridge connec-
tion. Note that it is suitable for any bridge application
where measurement speed is not of the utmost impor-
tance. For many applications where large vessels are
weighed, the average weight over an extended period of
time is of concern and short term weight is not readily
determined due to movement of contents, or mechanical
resonance.Often,largeweighingapplicationsinvolveload
The circuit in Figure 44 shows an example of a simple
amplification scheme. This example produces a differen-
tial output with a common mode voltage of 2.5V, as
determined by the bridge. The use of a true three amplifier
instrumentationamplifierisnotnecessary,astheLTC2413
LT1019
+
R1
2
V
REF
3
4
12
+
REF
REF
SDO
350Ω
BRIDGE
13
–
SCK
5
11
+
IN
CS
LTC2413
6
14
–
IN
F
O
GND
R2
1, 7, 8, 9,
10, 15, 16
2413 F43
R1 AND R2 CAN BE USED TO INCREASE TOLERABLE AC COMPONENT ON REF SIGNALS
Figure 43. Simple Bridge Connection
sn2413 2413fs
36
LTC2413
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has common mode rejection far beyond that of most
amplifiers. The LTC1051 is a dual autozero amplifier that
can be used to produce a gain of 15 before its input
referred noise dominates the LTC2413 noise. This ex-
ampleshowsagainof34, thatisdeterminedbyafeedback
network built using a resistor array containing 8 individual
resistors. The resistors are organized to optimize tem-
peraturetrackinginthepresenceofthermalgradients.The
second LTC1051 buffers the low noise input stage from
the transient load steps produced during conversion.
Figure 45 shows an example of a single amplifier used to
produce single-ended gain. This topology is best used in
applications where the gain setting resistor can be made
to match the temperature coefficient of the strain gauges.
If the bridge is composed of precision resistors, with only
one or two variable elements, the reference arm of the
bridgecanbemadetoactinconjunctionwiththefeedback
resistor to determine the gain. If the feedback resistor is
incorporated into the design of the load cell, using resis-
tors which match the temperature coefficient of the load-
cell elements, good results can be achieved without the
needforresistorswithahighdegreeofabsoluteaccuracy.
Thecommonmodevoltageinthiscase, isagainafunction
of the bridge output. Differential gain as used with a 350Ω
bridge is AV = (R1+ R2)/(R1+175Ω). Common mode gain
is half the differential gain. The maximum differential
signal that can be used is 1/4 VREF, as opposed to 1/2 VREF
in the 2-amplifier topology above.
The gain stability and accuracy of this approach is very
good, due to a statistical improvement in resistor match-
ing due to individual error contribution being reduced. A
gain of 34 may seem low, when compared to common
practiceinearliergenerationsofload-cellinterfaces, how-
ever the accuracy of the LTC2413 changes the rationale.
Achieving high gain accuracy and linearity at higher gains
may prove difficult, while providing little benefit in terms
of noise reduction.
Remote Half Bridge Interface
At a gain of 100, the gain error that could result from
typical open-loop gain of 160dB is –1ppm, however,
worst-case is at the minimum gain of 116dB, giving a gain
error of –158ppm. Worst-case gain error at a gain of 34,
is –54ppm. The use of the LTC1051A reduces the worst-
case gain error to –33ppm. The advantage of gain higher
than 34, then becomes dubious, as the input referred
noiseseeslittleimprovement1 andgainaccuracyispoten-
tially compromised.
As opposed to full bridge applications, typical half bridge
applications must contend with nonlinearity in the bridge
output,assignalswingisoftenmuchgreater.Applications
include RTD’s, thermistors and other resistive elements
that undergo significant changes over their span. For
singlevariableelementbridges, thenonlinearityofthehalf
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 46. The LTC2413 can accept inputs up
to 1/2 VREF. Hence, the reference resistor R1 must be at
least 2x the highest value of the variable resistor.
Note that this 4-amplifier topology has advantages over
the typical integrated 3-amplifier instrumentation ampli-
fier in that it does not have the high noise level common in
the output stage that usually dominates when an instru-
mentation amplifier is used at low gain. If this amplifier is
used at a gain of 10, the gain error is only 10ppm and input
referred noise is reduced to 0.1µVRMS. The buffer stages
canalsobeconfiguredtoprovidegainofupto50withhigh
gain stability and linearity.
In the case of 100Ω platinum RTD’s, this would suggest a
value of 800Ω for R1. Such a low value for R1 is not
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.
1Input referred noise for AV = 34 for approximately 0.05µVRMS, whereas at a gain of 50, it would be
0.048µVRMS
.
sn2413 2413fs
37
LTC2413
U
W U U
APPLICATIO S I FOR ATIO
The basic circuit shown in Figure 46 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 reference input, a low pass
filterisrecommendedasshowninFigure47.Notethatyou
cannot place a large capacitor directly at the junction of R1
and R2, as it will store charge from the sampling process.
Abetterapproachistoproducealowpassfilterdecoupled
from the input lines with a high value resistor (R3).
higher frequencies, will be reduced. A filter can be intro-
duced into the network, in the form of one or more
capacitors,orferritebeads,aslongasthesamplingpulses
are not translated into an error. The reference voltage is
alsoreduced, butthisisnotundesirable, asitwilldecrease
the value of the LSB, although, not the input referred noise
level.
The circuit shown in Figure 47 shows a more rigorous
example of Figure 46, with increased noise suppression
and more protection for remote applications.
Figure48showsanexampleofgainintheexcitationcircuit
and remote feedback from the bridge. The LTC1043’s
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
gainerrororduetooffsetvoltages.A1µV/°Coffsetvoltage
drift translates into 0.05ppm/°C gain error. Simpler alter-
natives, with the amplifiers providing gain using resistor
arrays for feedback, can produce results that are similar to
bridge sensing schemes via attenuators. Note that the
amplifiersmusthavehighopen-loopgainorgainerrorwill
The use of a third resistor in the half bridge, between the
variable and fixed elements gives essentially the same
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 100Ω RTD, the negative refer-
ence 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 re-
placed with a 10k 5% and a 10k 0.1% reference resistor,
the noise level introduced at the reference, at least at
5V
REF
0.1µF
5V
8
3
2
+
–
0.1µF
0.1µF
1
U1A
4
5V
2
8
2
3
350Ω
BRIDGE
–
+
V
CC
1
3
4
12
+
–
U2A
REF
REF
SDO
15
14
4
5
12
13
SCK
1
4
RN1
16
5
11
+
6
11
7
10
8
9
IN
CS
2
3
13
LTC2413
6
5
6
5
–
+
–
+
7
7
6
14
–
IN
U2B
U1B
F
O
GND
1, 7, 8, 9,
10, 15, 16
2413 F44
RN1 = 5k × 8 RESISTOR ARRAY
U1A, U1B, U2A, U2B = 1/2 LTC1051
Figure 44. Using Autozero Amplifiers to Reduce Input Referred Noise
sn2413 2413fs
38
LTC2413
U
W U U
APPLICATIO S I FOR ATIO
be a source of error. The fact that input offset voltage has
relatively little effect on overall error may lead one to use
low performance amplifiers for this application. Note that
the gain of a device such as an LF156, (25V/mV over
temperature) will produce a worst-case error of –180ppm
at a noise gain of 3, such as would be encountered in an
inverting gain of 2, to produce –10V from a 5V reference.
The circuits in Figures 48 and 50 could be used where
multiplebridgecircuitsareinvolvedandbridgeoutputcan
be multiplexed onto a single LTC2413, via an inexpensive
multiplexer such as the 74HC4052.
Figure 49 shows the use of an LTC2413 with a differential
multiplexer. This is an inexpensive multiplexer that will
contribute some error due to leakage if used directly with
the output from the bridge, or if resistors are inserted as
a protection mechanism from overvoltage. Although the
bridge output may be within the input range of the A/D and
multiplexer in normal operation, some thought should be
given to fault conditions that could result in full excitation
voltage at the inputs to the multiplexer or ADC. The use of
amplification prior to the multiplexer will largely eliminate
errors associated with channel leakage developing error
voltages in the source impedance.
The error associated with the 10V excitation would be
–80ppm. Hence, overall reference error could be as high
as 130ppm, the average of the two.
Figure 50 shows a similar scheme to provide excitation
using resistor arrays to produce precise gain. The circuit
is configured to provide 10V and –5V excitation to the
bridge, producing a common mode voltage at the input to
the LTC2413 of 2.5V, maximizing the AC input range for
applications where induced 60Hz could reach amplitudes
up to 2VRMS
.
5V
+
10µF
0.1µF
5V
350Ω
2
BRIDGE
0.1µV
V
7
CC
3
2
3
4
+
–
+
REF
REF
175Ω
1µF
6
LTC1050S8
+
–
20k
20k
5
+
+
4
IN
1µF
R1
4.99k
R2
46.4k
LTC2413
6
–
IN
GND
1, 7, 8, 9,
10, 15, 16
R1 + R2
2413 F45
A
= 9.95 =
V
(
)
R1 + 175Ω
Figure 45. Bridge Amplification Using a Single Amplifier
sn2413 2413fs
39
LTC2413
U
W U U
APPLICATIO S I FOR ATIO
V
S
2.7V TO 5.5V
2
V
CC
3
4
+
–
R1
25.5k
0.1%
REF
REF
LTC2413
5
6
+
IN
IN
PLATINUM
100Ω
RTD
–
GND
1, 7, 8, 9,
10, 15, 16
2413 F46
Figure 46. Remote Half Bridge Interface
5V
5V
2
R2
V
10k
CC
3
4
+
–
0.1%
REF
REF
+
R3
10k
5%
560Ω
1µF
R1
10k, 5%
LTC1050
–
LTC2413
10k
10k
5
6
+
IN
IN
PLATINUM
100Ω
–
RTD
GND
1, 7, 8, 9,
10, 15, 16
2413 F47
Figure 47. Remote Half Bridge Sensing with Noise Suppression on Reference
sn2413 2413fs
40
LTC2413
U
W U U
APPLICATIO S I FOR ATIO
15V
U1
15V
15V
7
LTC1043
4
200Ω
10V
5V
3
2
8
7
+
LT1236-5
10V
20Ω
*
6
+
+
Q1
2N3904
LTC1150
1µF
11
12
47µF
0.1µF
–
4
–15V
33Ω
14
13
10µF
0.1µF
1k
17
350Ω
BRIDGE
5V
0.1µF
2
V
CC
LTC2413
+
3
4
REF
–
REF
33Ω
5
6
+
IN
–
IN
U2
15V
7
GND
LTC1043
1, 7, 8, 9,
10, 15, 16
Q2
2N3906
3
2
5
15
8
6
+
*
6
LTC1150
2
3
20Ω
–
4
–15V
–15V
18
0.1µF
1k
*FLYING CAPACITORS ARE
1µF FILM (MKP OR EQUIVALENT)
5V
U2
LTC1043
4
SEE LTC1043 DATA SHEET FOR
DETAILS ON UNUSED HALF OF U1
7
*
11
12
1µF
FILM
200Ω
14
13
–10V
17
–10V
2413 F48
Figure 48. LTC1043 Provides Precise 4X Reference for Excitation Voltages
sn2413 2413fs
41
LTC2413
U
W U U
APPLICATIO S I FOR ATIO
5V
5V
+
16
2
47µF
12
14
15
11
V
CC
3
4
+
–
REF
REF
LTC2413
74HC4052
1
5
13
3
5
6
+
IN
IN
–
2
4
TO OTHER
DEVICES
GND
6
1, 7, 8, 9,
10, 15, 16
8
9
10
A0
A1
2413 F49
Figure 49. Use a Differential Multiplexer to Expand Channel Capability
sn2413 2413fs
42
LTC2413
U
PACKAGE DESCRIPTIO
GN Package
16-Lead Plastic SSOP (Narrow .150 Inch)
(Reference LTC DWG # 05-08-1641)
TOP VIEW
1
16
15
14
13
12
11
10
9
GND
GND
GND
V
2
CC
+
3
4
5
6
7
8
F
REF
REF
IN
O
–
+
–
SCK
SDO
CS
IN
GND
GND
GND
GND
GN PACKAGE
16-LEAD PLASTIC SSOP
sn2413 2413fs
Information furnished by Linear Technology Corporation is believed to be accurate and reliable.
However, no responsibility is assumed for its use. Linear Technology Corporation makes no represen-
tation that the interconnection of its circuits as described herein will notinfringe onexisting patent rights.
43
LTC2413
U
TYPICAL APPLICATIO
15V
5V
3
2
+
LT1236-5
20Ω
1/2
LT1112
1
+
Q1
2N3904
C3
47µF
C1
0.1µF
–
C1
0.1µF
22Ω
RN1
10k
10V
5V
1
2
3
2
RN1
10k
V
CC
4
350Ω BRIDGE
TWO ELEMENTS
VARYING
LTC2413
+
3
REF
4
–
REF
5
6
+
IN
–5V
–
IN
8
RN1
10k
GND
1, 7, 8, 9,
10, 15, 16
RN1
10k
7
5
6
15V
C2
0.1µF
33Ω
×2
RN1 IS CADDOCK T914 10K-010-02
8
6
–
Q2, Q3
2N3906
×2
20Ω
1/2
LT1112
7
5
+
4
–15V
2413 F50
–15V
Figure 50. Use Resistor Arrays to Provide Precise Matching in Excitation Amplifier
RELATED PARTS
PART NUMBER
DESCRIPTION
COMMENTS
LT1019
Precision Bandgap Reference, 2.5V, 5V
Micropower Thermocouple Cold Junction Compensator
3ppm/°C Drift, 0.05% Max Initial Accuracy
80µA Supply Current, 0.5°C Initial Accuracy
Precise Charge, Balanced Switching, Low Power
LT1025
LTC1043
Dual Precision Instrumentation Switched Capacitor
Building Block
LTC1050
Precision Chopper Stabilized Op Amp
Precision Bandgap Reference, 5V
No External Components 5µV Offset, 1.6µV Noise
P-P
LT1236A-5
LT1460
0.05% Max Initial Accuracy, 5ppm/°C Drift
Micropower Series Reference
0.075% Max, 10ppm/°C Max Drift
LTC2400
24-Bit, No Latency ∆Σ ADC in SO-8
1-/2-Channel, 24-Bit, No Latency ∆Σ ADC in MSOP
4-/8-Channel, 24-Bit, No Latency ∆Σ ADC
0.3ppm Noise, 4ppm INL, 10ppm Total Unadjusted Error, 200µA
0.6ppm Noise, 4ppm INL, 10ppm Total Unadjusted Error, 200µA
0.3ppm Noise, 4ppm INL, 10ppm Total Unadjusted Error, 200µA
LTC2401/LTC2402
LTC2404/LTC2408
LTC2410
24-Bit, Fully Differential, No Latency ∆Σ ADC in SSOP-16 0.16ppm Noise, 2ppm INL, 3ppm Total Unadjusted Error, 200µA
LTC2411
24-Bit, Fully Differential, No Latency ∆Σ ADC in MS10
24-Bit, Fully Differential, ∆Σ ADC
0.29ppm Noise, 2ppm INL, 3ppm Total Unadjusted Error, 200µA
15Hz Output Rate at 60Hz Rejection, Pin Compatible with LTC2410
1.2ppm Noise, 8ppm INL, Pin Compatible with LTC2400
LTC2415
LTC2420
20-Bit, No Latency ∆Σ ADC in SO-8
LTC2424/LTC2428
4-/8-Channel, 20-Bit, No Latency ∆Σ ADC
1.2ppm Noise, 8ppm INL, Pin Compatible with LTC2404/LTC2408
sn2413 2413fs
LT/TP 0501 4K • PRINTED IN USA
44 LinearTechnology Corporation
1630 McCarthy Blvd., Milpitas, CA 95035-7417
●
●
(408)432-1900 FAX:(408)434-0507 www.linear-tech.com
LINEAR TECHNOLOGY CORPORATION 2000
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