DN207 - LTC2400 High Accuracy Differential to Single-Ended Converter for ±5V Supplies

LTC2400 High Accuracy Differential to Single-Ended
Converter for ±5V Supplies – Design Note 207
Differential to Single-Ended Converter Has Very High
Uncalibrated Accuracy and Low Offset and Drift
Kevin R. Hoskins and Derek V Redmayne
Introduction
The circuit in Figure 1 is ideal for low level differential
signals in applications that have a ±5V supply and need
high accuracy without calibration. The circuit achieves
19.6-bit resolution and 18.1-bit accuracy. These and
other specifications are summarized in Table 1.
Operation
The circuit in Figure 1 combines an LTC ®1043 and
LTC1050 as a differential to single-ended amplifier
that has an input common mode range that includes
the power supplies. It uses the LTC1043 to sample a
differential input voltage, holds it on CS and transfers
it to a ground-referred capacitor, CH. The voltage on
CH is applied to the LTC1050’s noninverting input and
5V
0.1μF
amplified by the gain set by resistors R1 and R2 (101
for the values shown). The amplifier’s output is then
converted to a digital value by the LTC2400.
The LTC1043 achieves its best differential to singleended conversion when its internal switching frequency
operates at a nominal 300Hz, as set by the 0.01μF
capacitor C1 and when 1μF capacitors are used for CS
and CH. CS and CH should be a film type such as mylar
or polypropylene. Conversion accuracy is enhanced
by placing a guard shield around CS and connecting
the shield to Pin 10 of the LTC1043. This minimizes
nonlinearity that results from stray capacitance transfer
errors associated with CS. To minimize the possibility of
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OPTIONAL GUARD CIRCUIT FOR CH
R4
R3
90.9Ω
9.09k
5V
BRIDGE—
TYPICAL
INPUT
0.1μF
8
2
350Ω
DIFFERENTIAL
INPUT
11
10
+
CS
1μF
(EXT)
+
7
–
6
RS*
5.1k
3
VIN
LTC2400
GND
0.1μF
R1
9.09k
R2
90.9Ω
12
CS
VREF
SDO
SCK
4
CH
1μF
–5V
350Ω
AGND OR
–VEXT
1
VCC
2
3
LTC1050
350Ω
0.1μF
4
7
350Ω
VREFIN 5V
1/2 LTC1043
SINGLE-POINT OR “STAR” GROUND
0.1μF
–5V
Figure 1. Differential to Single-Ended Converter for Low Level Inputs,
Such as Bridges, Maintains the LTC2400’s High Accuracy
07/99/207_conv
SERIAL DATA OUT
SERIAL CLOCK
*OPTIONAL—LIMITS INPUT CURRENT
IF THE INPUT VOLTAGE GOES BELOW
–300mV
R1, R2 = 0.02% INITIAL TOLERANCE OR BETTER
R3, R4 = 1%
16
17
7
CHIP SELECT
8
DN207 F01
C1
0.01μF
6
FO
4
14
13
5
PCB leakage currents introducing an error source into
CH, an optional guard circuit could be added as shown.
The common point of these two resistors produces the
potential for the guard ring. Consult the LTC1043 data
sheet for more information. As is good practice in all
high precision circuits, keep all lead lengths as short as
possible to minimize stray capacitance and noise pickup.
The LTC1050’s closed-loop gain accuracy is affected by
the tolerance of the ratio of the gain-setting resistors.
If cost considerations preclude using low tolerance
resistors (0.02% or better), the processor to which the
LTC2400 is connected can be used to perform software
correction. Operated as a follower, the LTC1050’s gain
and linearity error is less than 0.001%.
As stated above, the LTC1043 has the highest transfer
accuracy when using 1.0μF capacitors. For example,
0.1μF will typically increase the circuit’s overall nonlinearity tenfold to 0.001% or 10ppm.
A source of errors is thermocouple effects that occur
in soldered connections. Their effects are most pronounced in the circuit’s low level portion, before the
LTC1050’s output. Any temperature changes in any of
the low level circuitry’s connections will cause linearity
perturbations in the final conversion result. Their effects can be minimized by balancing the thermocouple
connections with reversed redundant connections and
by sealing the circuit against moving air.
A subtle source of error arises from ground lead
impedance differences between the LTC1043 circuit,
the LTC1050 preamplifier and the LTC2400. This error
can be avoided by connecting Pin 14 of the LTC1043,
the bottom end of R2 and Pin 4 of the LTC2400 to a
single-point “star” ground.
The circuit’s input current consists of common mode
and differential mode components. The differential
mode input current can be as much as ±25nA when
VIN(CM) is equal to the + or –5V common mode limit,
and VDIFF is 40mV (typ). The ratio of common mode
to differential input current is nominally 3:1. Under
balanced input conditions (VIN(CM) = 0), the total input
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current is typically 1nA. The values may vary from part
to part. Figure 1’s input is analogous to a 2μF capacitor in parallel with a 25MΩ connected to ground. The
LTC1043’s nominal 800Ω switch resistance is between
the source and the 2μF capacitance.
The circuit schematic shows an optional resistor, RS.
This resistor can be placed in series with the LTC2400’s
input to limit current if the input goes below –300mV.
The resistor does not degrade the converter’s performance as long as any capacitance, stray or otherwise,
connected between the LTC2400’s input and ground is
less than 100pF. Higher capacitance will increase offset
and full-scale errors.
Other differential to single-ended conditioning circuits
for the LTC2400 are available on LTC’s web site. Refer
to the URL at the bottom of this page.
Table 1. Performance Specifications for Figure 1’s
Circuit. VCC = VREF = LT®1236-5; VFS = 40mV,
RSOURCE = 175Ω (Balanced)
CIRCUIT
(MEASURED) LTC2400
PARAMETER
Input Voltage Range
–3 to 40
Zero Error
12.7
TOTAL
(UNITS)
mV
1.5
μV
Input Current
See Text
Nonlinearity
±1
4
ppm
Input-Referred Noise
(without averaging)
0.3*
1.5
μVRMS
Input-Referred Noise
(averaged 64 readings)
0.05*
μVRMS
Resolution (with
averaged readings)
19.6
Bits
Overall Accuracy
(uncalibrated**)
18.1
Bits
Supply Voltage
±5
5
V
Supply Current
1.6
0.2
mA
CMRR
120
dB
Common Mode Range
±5
V
*Input-referred noise with a gain of 101.
**Does not include gain setting resistors.
For applications help,
call (408) 432-1900
dn207f_conv LT/TP 0799 370K • PRINTED IN THE USA
1630 McCarthy Blvd., Milpitas, CA 95035-7417
(408) 432-1900
●
FAX: (408) 434-0507 ● www.linear.com
© LINEAR TECHNOLOGY CORPORATION 1999