LINEAR TECHNOLOGY LT5400 Technical data

Matched Resistor Networks for Precision Amplifi er Applications
Design Note 502
Tyler Hutchison
Introduction
Some ideal op amp confi gurations assume that the feedback resis tors exhibit perfec t matching. In practice, resistor non-idealities can af fect various circuit param­eters such as common mode rejection ratio (CMRR), harmonic distortion and stability. For instance, as shown in Figure 1, a single-ended amplifi er confi gured to level-shift a ground-referenced signal to a common mode of 2.5V needs a good CMRR. Assuming 34dB CMRR and no input signal, this 2.5V level shi fter exhibits an output offset of 50mV, which can even overwhelm the LSB and offset errors of 12-bit ADCs and drivers.
R
V
LTC6255
+
CC
+
DN502 F01
V
EE
R
+
V
IN
R
2.5V
+
R
DC
Figure 1. A Single-Ended Op Amp Used as a Level Shifter
For an op amp, 34dB is a less than ide al CMRR. However, a feedback network of 1% tolerance resistors can limit the CMRR to 34dB regardless of the op amp’s capabili­ties. Highly matched resistors, such as those provided
®
by the LT
5400, available in 0.01%, 0.025% and 0.05% matching, ensure that the designer can approach or meet amplifi er data sheet specifi cations. This design note compares the LT5400 with thick fi lm, 0402, 1% tolerance surface mount resistors. CMRR, harmonic distortion and stability are considered with these resis­tors for feedback around an LTC6362 op amp, as shown in Figure 2.
Common Mode Rejection Ratio
In order to obtain precis e measurements in the presence of common mode noise, a high CMRR is important. Input CMRR is defi ned as the ratio of differential gain (V
OUT(DIFF)/VIN(DIFF)
differential conversion (V
) to the input common mode to
OUT(DIFF)/VIN(CM)
).
R2 1k
LTC6362
+
5V
+
R3 1k
50Ω
50Ω
3.3nF
3.3nF
3.3nF
DN502 F02
+
A
IN
TO ADC
A
IN
R1 5k
+V
IN
R4 5k
–V
IN
Figure 2. Fully Differential Op Amp Confi gured for V
OUT/VIN
= 0.2
In ideal single-ended and fully differential amplifi ers, only the input differential level affects the output volt­age. However, in real circuits, resistor mismatch limits the available CMRR. Consider this circuit confi gured to attenu ate a ±10V signal to a ±2V signal. Using t ypical sur­face mount resistors with 2% matching (1% tolerance), the worst-case CMRR contribution from the resistors is 30dB. With 0.01% tolerance, 0.02% matching, the worst-case CMRR contribution from the resistors is 70dB. A limiting factor in the CMRR equation is:
R3
⎛ ⎜
R2
R2
R4
R1
12R1
This expression r educes to the resistor matching r atio for typic al resistors, but the LT5400 t akes an additional step to offer improved CMRR by constraining the matching between resistor pairs R1/R2 and R4/R3. By defi ning this equation as matching for CMRR, the LT5400 offers accuracy that’s better than just the resistor matching ratio. For example, the LT5400A guarantees:
R
R
0.005%
CMRR
which improves worst-case CMRR to 82dB.
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05/12/502
A bench test of the circuit yielded a CMRR of 50.7dB (highly resistor matching limited) with 1% tolerance resistors, and 86.6dB with the LT5400. In this case, a 2.5V common mode input would result in an offset of 1.5mV with 1% thick-fi lm resistors and an offset of 23μV with the LT5400, making it suitable for 18-bit ADC applications where DC accuracy is critical.
Harmonic Distortion
Harmonic distortion is also important when choosing resistors for a precision application. A large-signal voltage across a resistor may signifi cantly change the resistance depending on the size and material. This p r o b l e m o c c u r s i n a n u m b e r o f c h i p - b a s e d r e s i s t o r s , a n d naturally becomes more severe as the power levels at the resistors increase. Table 1 compares the distortion of thick fi lm, through-hole, and the LT5400 resistors based on high power drive and similar power drive. The results suggest that for a given signal, the LT5400 distorts the signal much less than other resistor types.
Stability
Figure 3 shows a model of the distributed capacitance between resistors in the LT5400. To achieve high preci­sion matching and tracking in the LT5400, many small SiCr resistors are confi gured in series and parallel. As a result of the complex interdigitation, the LT5400 resistors can be modeled as a series of infi nitesimal resistors with parasitic capacitance between adjacent segments and between individual segments and the ex­posed pad. In contra st, typical sur face mount resistors, without the tight layout, typically exhibit signifi cantly less parasitic capacitance.
The ef fect of inter-r esistor capacitance c an be mitigated when the exposed pad is grounded. However, even after grounding the exposed pad, this capacitance still
EXPOSED PAD
EXPOSED
EXPOSED
INTER
EXPOSED
EXPOSED
INTER
EXPOSED PAD
EXPOSED
EXPOSED
INTER
ttt
EXPOSED
EXPOSED
INTER
DN502 F03
Figure 3. A Simple Model of the Distributed Capacitance in a Matched Resistor IC. The Sum of R Components Creates an Equivalent Single Resistor. The Net Effect of C
is 1.4pF and the Net Effect of C’
INTER
EXPOSED
is 5.5pF
affec ts circuit stabilit y by forming a parasitic pole on the order of the total resistance times the total capacitance.
Since overshoot is inver sely proportional to phase mar­gin, minimizing step response overshoot is a good way to ensure circuit stability. The uncompensated LT5400 confi gura tion exhibits 27% compared to 17% overshoot from the 0402 confi guration. However, the compensa­tion capacitor necessary to achieve 8% overshoot is approximately the same in both confi gurations: 18pF with the LT5400; 15pF with 0402 resistors. With nearly identical compensation, the two circuits display similar stability characteristics.
Conclusion
The actual performance of precision amplifi ers and ADCs is often diffi cult to achieve since data sheet specifi cations assume ideal components. Carefully matched resistor networks, such as those supplied by the LT5400, enable precision matching orders of magnitude better than discrete components, ensuring data sheet specifi cations are met for precision ICs.
Table 1. For a Given Power Level, the LT5400 Behaves More Linearly Than Other Resistor Types
SOURCE HD3 –120.00 AT MAX POWER (12V
RESISTOR TYPE POWER RATING HD3 (56mW POWER) HD3 (1/14th RATED POWER)
LT5400 0.8W –117dBc –117dBc 5% Through-Hole 0.25W –100dBc –114dBc 1% Through-Hole 0.25W –115dBc –119dBc
1206 Thick Film 0.25W –104dBc –115dBc 0805 Thick Film 0.125W –93dBc –117dBc 0603 Thick Film 0.1W –89dBc –117dBc 0402 Thick Film 0.068W –72dBc –104dBc
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= 56mW into 1kΩ)
RMS
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