LINEAR TECHNOLOGY LTC6081 Technical data

DESIGN IDEAS L
V
RRR
R
V V
OUT IN IN
= +
 
 
 
 
( )
1
2 105
3
2 1
V V V
V
R
R
V V
OS OSB OSA
OSC
OSB OSA
= +
+
1
2 1
0
+
V
OUT
V
IN1
+
LTC6081/2
A
LTC6081/2
C
R4R3
V
IN2
+
LTC6081/2
B
R6R5
+
V
OUT
V
IN1
+
LTC6081/2
A
LTC6081/2
C
R4R3
R1
V
IN2
+
LTC6081/2
B
R6R5
R2
R0
V
OSDRIFT
(µV/°C)
NUMBER OF AMPLIFIERS (OUT OF 100)
30
25
20
15
10
5
0
LTC6081MS8 TA = –40°C TO 125°C VS = 3V VCM = 0.5V
0.20 0.30–0.10–0.20 0 0.10
CMOS Op Amp Outperforms Bipolar Amps in Precision Applications
Introduction
The LTC6081 and LTC6082 are dual and quad low offset, low drift, low noise CMOS operational amplifiers with rail­to-rail input and output stages. Their
0.8µV/°C maximum offset drift, 1pA input bias current, 1.3µV 10Hz noise, 120dB open loop gain and 110dB CMRR and PSRR make them perfect for precision applications. The LTC6081 and LTC6082 have a gain bandwidth product of 3.6MHz, with each amplifier only consuming about 330µA current for a supply voltage of
2.7 to 5.5V. The 10-lead DFN pack­age of the LTC6081 offers a shutdown function to reduce each amplifier’s supply current to 2µA.
Superior Precision CMOS Op Amp
Bipolar amplifiers can have low offset and low offset drift, but their nA level input bias current make them inap­propriate for high input impedance applications such as photodiode amplifiers. CMOS amplifiers usually offer inferior offset drift, CMRR, and PSRR specifications and therefore are not suitable for precision applica­tions. Chopper stabilized amplifiers, also known as zero drift amplifiers, can achieve superior offset and offset drift by means of offset cancellation, but have clock noise and fold-back noise due to sampling. LTC6081 and LTC6082, however, are continuous time CMOS operational amplifiers, which use a patented methodology to improve their offset voltage, offset voltage drift and CMRR. They combine the features of low input bias current, low offset drift and low noise.
Instrumentation Amplifier
Figure 2 shows a typical three op amp instrumentation amplifier. If R1 = R2, R3 = R5 and R4 = R6, then
Linear Technology Magazine • March 2008
by Hengsheng Liu
R4/R3 and R6/R5 is critical for CMRR. Gain can be changed by simply chang­ing R0 without affecting the resistor matching.
The input referred offset of the
of 0.1Hz to
p-p
Figure 1. VOS drift histogram of LTC6081
In this two stage structure, the dif­ferential voltage passes through the first gain stage with gain of 1 + 2R1/R0 while the common mode voltage has only unity gain at the first stage, thus improving CMRR. Ratio matching of
Figure 2. Typical three op amp structure of instrumentation amplifier
Figure 3. Instrumentation amplifier with unity gain buffers
amplifier is
Statistically, the total VOS is √2 times the VOS of a single op amp. Since a single LTC6081 op amp drifts less than 0.8µV/°C, the amplifier in Figure 2 will drift less than 1.1µV/°C. One drawback of the circuit in Figure 2 is its common mode operating range is no longer rail-to-rail. Assuming
3535
L DESIGN IDEAS
R R
R R
6 5
1
4 3
= +
( )
ε
20log
A
V
ε
V V
R
R
V V
IN CM IN DM
( ) ( )
< ± <
+
2
1
0
V
R
R
V V
V
R
R
V
IN DM IN CM
IN DM
( ) ( )
( )
+ < <
+
2
2
1
0
1
0
+
V
OUT
V
IN1
LTC6081/2
R4R3
V
IN2
R6R5
5V
5V
+
+
1M
1M
10k
0.1µF
1µF
2.49M
V
OUT
= 10mV/°C
0°C TO 500°C
100pF
K
LT1025
R
SENSOR: OMEGA 5TC-TT-K-30-36 K-TYPE THERMOCOUPLE 1M RESISTORS PROTECT CIRCUIT TO ±350V WITH NO PHASE REVERSAL OF AMPLIFIER OUTPUT 1pA MAX I
BIAS
TRANSLATES TO 0.05°C ERROR
90µV VOS 2°C OFFSET
1/2
LTC6081
the differential and common mode input voltage are V
IN(DM)
and V
IN(CM)
respectively, the output voltages of op amp A and B are then V R0)V
IN(DM)
and V
+ (2R1/R0)V
IN(CM)
IN(CM)
– (2R1/
IN(DM)
respectively. So
where V+ and V– are the positive and negative supply voltage respectively. The larger the first stage gain or input differential signal is, the narrower the input common mode range is. To widen the input common mode range, the first stage gain can be reduced, but this will compromise CMRR per­formance.
Figure 3 is a reduced circuit of Fig­ure 2 with a unity gain buffer at the front stage. This circuit can achieve rail-to-rail input range. As mentioned
previously, it won’t have the high CMRR of the circuit in Figure 2 since we reduced the front stage gain to unity. If the input resistance require­ment can be eased, Figure 3 can be reduced to Figure 4, a single stage difference amplifier. The impedance of the non-inverting and inverting inputs are R3 and R5 + R6, respectively. An obvious advantage of the LTC6081 is its super low input bias current. Even with a 1M input resistor R3 or R5, the less than 1pA input bias current of LTC6081 will add less than 1µV to VOS.
The above discussion assumes a perfect matching of R4/R3 and R6/R5. If
then the CMRR degrades to
where AV is the differential gain of the instrumentation amplifier. For example, at gain of 10, to achieve 80dB
Figure 4. Difference amplifier with no input buffers
CMRR, mismatch of R4/R3 and R6/R5 should be less than 0.1%. This is true for all the above three circuits. The advantage of the circuit in Figure 2 is that gain can be put at the front stage to ease the matching requirements of the second stage. Matching of R1 and R2 in Figure 2 is not important.
Thermocouple Amplifier
Figure 5 shows the LTC6081 in a thermocouple amplifier. The 1M re­sistors protect the circuit up to ±350V with no phase reversal to amplifier output. The 1pA maximum IBIAS of the LTC6081 translates to a miniscule
0.05°C temperature error with the 1M input protection resistor. The ±90µV offset over the entire operating temperature range ensures a less than 2°C temperature offset.
LTM4605/07, continued from page 19
Conclusion
The LTM4605 and LTM4607 µModule regulators simplify the design of buck­boost power supplies. Their low profile 15mm × 15mm × 2.8mm packages and minimal component count help free up valuable PCB area. High input and high output ratings suit these
36
36
Figure 5. Thermocouple amplifier
regulators to networking, industrial, automotive systems and high power battery-operated devices. Their opti­mized internal 4-switch architecture provides high efficiency and high performance. Overall, the LTM4605 and LTM4607 reduce product design and test time with a mix of high per-
Conclusion
The LTC6081 and LTC6082 are high performance dual and quad op amps combining excellent noise, offset drift, CMRR, PSRR and input bias current specifications. They perform in a vari­ety of topologies without compromising performance. LTC6081 is available in 8-lead MSOP and 10-lead DFN pack­ages. LTC6082 is available in 16-lead SSOP and DFN packages.
formance features, flexible settings and ease-of-use.
Notes
1 For more about layout with Kelvin sense resis-
tors, see “Using Current Sensing Resistors with Hot Swap Controllers and Current Mode Voltage Regulators” by Eric Trelewicz in Linear Technology
Magazine, September 2003, page 34
Linear Technology Magazine • March 2008
L
L
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