Datasheet LMP7732MA, LMP7732 Datasheet (NSC)

August 2007
LMP7732
2.9 nV/sqrt(Hz) Low Noise, Precision, RRIO Amplifier
General Description
The LMP7732 is a dual low noise, low offset voltage, rail-to­rail input and output, low voltage precision amplifier. The LMP7732 is part of the LMP® precision amplifier family and is ideal for precision and low noise applications with low voltage requirements.
This operational amplifier offers low voltage noise of 2.9 nV/
with a 1/f corner of only 3 Hz and low DC offset with a maximum value of ±40 µV, targeting high accuracy, low fre­quency applications. The LMP7732 has bipolar junction input stages with a bias current of only 1.5 nA. This low input bias current, complemented by the very low AC and DC levels of voltage noise, makes the LMP7732 an excellent choice for photometry applications.
The LMP7732 provides a wide GBW of 22 MHz while con­suming only 4 mA of current. This high gain bandwidth along with the high open loop gain of 130 dB enables accurate sig­nal conditioning in applications with high closed loop gain requirements.
The LMP7732 has a supply voltage range of 1.8V to 5.5V, making it an ideal choice for battery operated portable appli­cations.
The LMP7732 is offered in an 8-pin SOIC. The LMP7731 is the single version of this product and is of-
fered in an 5-Pin SOT23 package.
Features
(Typical values, TA = 25°C, VS = 5V)
Input voltage noise
f = 3 Hz 3.3 nV/Hz
f = 1 kHz 2.9 nV/Hz
Offset voltage (max) ±40 µV
Offset voltage drift (max) ±1.3 µV/°C
CMRR 130 dB
Open loop gain 130 dB
GBW 22 MHz
Slew rate 2.4 V/µs
THD @ f = 10 kHz, AV = 1, RL = 2 k 0.001%
Supply current 4.4 mA
Supply voltage range 1.8V to 5.5V
Operating temperature range −40°C to 125°C
Input bias current ±1.5 nA
RRIO
8-Pin SOIC package
Applications
Thermopile amplifier
Gas analysis instruments
Photometric instrumentation
Medical instrumentation
Typical Application
Thermopile Signal Amplifier
30015001
LMP® is a registered trademark of National Semiconductor Corporation.
© 2007 National Semiconductor Corporation 300150 www.national.com
LMP7732 Low Noise, Precision, RRIO Amplifier
Absolute Maximum Ratings (Note 1)
If Military/Aerospace specified devices are required, please contact the National Semiconductor Sales Office/ Distributors for availability and specifications.
ESD Tolerance (Note 2) Human Body Model For inputs pins only 2000V For all other pins 2000V Machine Model 200V Charge Device Model 1000V VIN Differential
±2V
Supply Voltage (VS = V+ – V−)
6.0V
Storage Temperature Range −65°C to 150°C Junction Temperature (Note 3) +150°C max Soldering Information Infrared or Convection (20 sec) 235°C Wave Soldering Lead Temp. (10 sec) 260°C
Operating Ratings (Note 1)
Temperature Range −40°C to 125°C Supply Voltage (VS = V+ – V–)
1.8V to 5.5V
Package Thermal Resistance (θJA)
8-Pin SOIC 190 °C/W
2.5V Electrical Characteristics (Note 4)
Unless otherwise specified, all limits are guaranteed for TA = 25°C, V+ = 2.5V, V− = 0V, VCM = V+/2, RL >10 k to V+/2. Bold­face limits apply at the temperature extremes.
Symbol Parameter Conditions Min
(Note 6)
Typ
(Note 5)
Max
(Note 6)
Units
V
OS
Input Offset Voltage (Note 7)
VCM = 2.0V ±9 ±50
±150
μV
VCM = 0.5V ±9 ±40
±125
TCV
OS
Input Offset Voltage Drift VCM = 2.0V ±0.5 ±1.3
μV/°C
VCM = 0.5V ±0.2 ±0.8
Input Offset Voltage Time Drift VCM = 0.5V and VCM = 2.0V 0.35
μV/month
I
B
Input Bias Current VCM = 2.0V ±1 ±30
±45
nA
VCM = 0.5V ±12 ±50
±75
I
OS
Input Offset Current VCM = 2.0V ±1 ±50
±75
nA
VCM = 0.5V ±11 ±60
±80
TCI
OS
Input Offset Current Drift VCM = 0.5V and VCM = 2.0V 0.0474 nA/°C
CMRR Common Mode Rejection Ratio
0.15V VCM 0.7V
0.23V VCM 0.7V
101
89
120
dB
1.5V VCM 2.35V
1.5V VCM 2.27V
105
99
129
PSRR Power Supply Rejection Ratio
2.5V V+ 5V
111
105
129
dB
1.8V V+ 5.5V
117
CMVR Input Common-Mode Voltage
Range
Large Signal CMRR 80 dB
0
2.5 V
A
VOL
Large Signal Voltage Gain
RL = 10 k to V+/2 VO = 0.5V to 2.0V
112
104
130
dB
RL = 2 k to V+/2 VO = 0.5V to 2.0V
109
90
119
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LMP7732
Symbol Parameter Conditions Min
(Note 6)
Typ
(Note 5)
Max
(Note 6)
Units
V
O
Output Swing High
RL = 10 k to V+/2
4 50
75
mV
from either
rail
RL = 2 k to V+/2
13 50
75
Output Swing Low
RL = 10 k to V+/2
6 50
75
RL = 2 k to V+/2
9 50
75
I
O
Output Short Circuit Current Sourcing, VO = V+/2
VIN (diff) = 100 mV
22
12
31
mA
Sinking, VO = V+/2 VIN (diff) = −100 mV
15
10
44
I
S
Supply Current VCM = 2.0V 4.0 5.4
6.8
mA
VCM = 0.5V 4.6 6.2
7.8
SR Slew Rate
AV = +1, CL = 10 pF, RL = 10 k to V+/2 VO = 2 V
PP
2.4
V/μs
GBW Gain Bandwidth Product
CL = 20 pF, RL = 10 k to V+/2
21 MHz
G
M
Gain Margin
CL = 20 pF, RL = 10 k to V+/2
14 dB
Φ
M
Phase Margin
CL = 20 pF, RL = 10 k to V+/2
60 deg
R
IN
Input Resistance Differential Mode 38
k
Common Mode 151
M
THD Total Harmonic Distortion AV = 1, fO = 1 kHz, Amplitude = 1V 0.002
%
e
n
Input-Referred Voltage Noise f = 1 kHz, VCM = 2.0V 3.0
nV/
f = 1 kHz, VCM = 0.5V 3.0
0.1 Hz to 10 Hz 75 nV
PP
i
n
Input-Referred Current Noise f = 1 kHz, VCM = 2.0V 1.1
pA/
f = 1 kHz, VCM = 0.5V 2.3
3.3V Electrical Characteristics (Note 4)
Unless otherwise specified, all limits are guaranteed for TA = 25°C, V+ = 3.3V, V− = 0V, VCM = V+/2, RL > 10 k to V+/2. Bold­face limits apply at the temperature extremes.
Symbol Parameter Conditions Min
(Note 6)
Typ
(Note 5)
Max
(Note 6)
Units
V
OS
Input Offset Voltage (Note 7)
VCM = 2.5V ±6 ±50
±150
μV
VCM = 0.5V ±6 ±40
±125
TCV
OS
Input Offset Voltage Drift VCM = 2.5V ±0.5 ±1.3
μV/°C
VCM = 0.5V ±0.2 ±0.8
Input Offset Voltage Time Drift VCM = 0.5V and VCM = 2.5V 0.35
μV/month
I
B
Input Bias Current VCM = 2.5V ±1.5 ±30
±45
nA
VCM = 0.5V ±13 ±50
±77
I
OS
Input Offset Current VCM = 2.5V ±1 ±50
±70
nA
VCM = 0.5V ±11 ±60
±80
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LMP7732
Symbol Parameter Conditions Min
(Note 6)
Typ
(Note 5)
Max
(Note 6)
Units
TCI
OS
Input Offset Current Drift VCM = 0.5V and VCM = 2.5V 0.048 nA/°C
CMRR Common Mode Rejection Ratio
0.15V VCM 0.7V
0.23V VCM 0.7V
101
89
120
dB
1.5V VCM 3.15V
1.5V VCM 3.07V
105
99
130
PSRR Power Supply Rejection Ratio
2.5V V+ 5.0V
111
105
129
dB
1.8V V+ 5.5V
117
CMVR Input Common-Mode Voltage
Range
Large Signal CMRR 80 dB
0
3.3 V
A
VOL
Large Signal Voltage Gain
RL = 10 k to V+/2 VO = 0.5V to 2.8V
112
104
130
dB
RL = 2 k to V+/2 VO = 0.5V to 2.8V
110
92
119
V
O
Output Swing High
RL = 10 k to V+/2
5 50
75
mV
from either
rail
RL = 2 k to V+/2
14 50
75
Output Swing Low
RL = 10 k to V+/2
9 50
75
RL = 2 k to V+/2
13 50
75
I
O
Output Short Circuit Current Sourcing, VO = V+/2
VIN (diff) = 100 mV
28
22
45
mA
Sinking, VO = V+/2 VIN (diff) = −100 mV
25
20
48
I
S
Supply Current VCM = 2.5V 4.2 5.6
7.0
mA
VCM = 0.5V 4.8 6.4
8.0
SR Slew Rate
AV = +1, CL = 10 pF, RL = 10 k to V+/2 VO = 2 V
PP
2.4
V/μs
GBW Gain Bandwidth Product
CL = 20 pF, RL = 10 k to V+/2
22 MHz
G
M
Gain Margin
CL = 20 pF, RL = 10 k to V+/2
14 dB
Φ
M
Phase Margin
CL = 20 pF, RL = 10 k to V+/2
62 deg
THD Total Harmonic Distortion AV = 1, fO = 1 kHz, Amplitude = 1V 0.002
%
R
IN
Input Resistance Differential Mode 38
k
Common Mode 151
M
e
n
Input-Referred Voltage Noise f = 1 kHz, VCM = 2.5V
2.9 nV/
f = 1 kHz, VCM = 0.5V
2.9
0.1 Hz to 10 Hz 75 nV
PP
i
n
Input-Referred Current Noise f = 1 kHz, VCM = 2.5V 1.1
pA/
f = 1 kHz, VCM = 0.5V 2.1
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LMP7732
5V Electrical Characteristics (Note 4)
Unless otherwise specified, all limits are guaranteed for TA = 25°C, V+ = 5V, V− = 0V, VCM = V+/2, RL > 10 k to V+/2. Boldface limits apply at the temperature extremes.
Symbol Parameter Conditions Min
(Note 6)
Typ
(Note 5)
Max
(Note 6)
Units
V
OS
Input Offset Voltage (Note 7)
VCM = 4.5V ±6 ±50
±150
μV
VCM = 0.5V ±6 ±40
±125
TCV
OS
Input Offset Voltage Drift VCM = 4.5V ±0.5 ±1.3
μV/°C
VCM = 0.5V ±0.2 ±0.8
Input Offset Voltage Time Drift VCM = 0.5V and VCM = 4.5V 0.35
μV/month
I
B
Input Bias Current VCM = 4.5V ±1.5 ±30
±50
nA
VCM = 0.5V ±14 ±50
±85
I
OS
Input Offset Current VCM = 4.5V ±1 ±50
±70
nA
VCM = 0.5V ±11 ±65
±80
TCI
OS
Input Offset Current Drift VCM = 0.5V and VCM = 4.5V 0.0482 nA/°C
CMRR Common Mode Rejection Ratio
0.15V VCM 0.7V
0.23V VCM 0.7V
101
89
120
dB
1.5V VCM 4.85V
1.5V VCM 4.77V
105
99
130
PSRR Power Supply Rejection Ratio
2.5V V+ 5V
111
105
129
dB
1.8V V+ 5.5V
117
CMVR Input Common-Mode Voltage
Range
Large Signal CMRR 80 dB
0
5 V
A
VOL
Large Signal Voltage Gain
RL = 10 k to V+/2 VO = 0.5V to 4.5V
112
104
130
dB
RL = 2 k to V+/2 VO = 0.5V to 4.5V
110
94
119
V
O
Output Swing High
RL = 10 k to V+/2
8 50
75
mV
from either
rail
RL = 2 k to V+/2
24 50
75
Output Swing Low
RL = 10 k to V+/2
9 50
75
RL = 2 k to V+/2
23 50
75
I
O
Output Short Circuit Current Sourcing, VO = V+/2
VIN (diff) = 100 mV
33
27
47
mA
Sinking, VO = V+/2 VIN (diff) = −100 mV
30
25
49
I
S
Supply Current VCM = 4.5V 4.4 6.0
7.4
mA
VCM = 0.5V 5.0 6.8
8.4
SR Slew Rate
AV = +1, CL = 10 pF, RL = 10 k to V+/2 VO = 2 V
PP
2.4
V/μs
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LMP7732
Symbol Parameter Conditions Min
(Note 6)
Typ
(Note 5)
Max
(Note 6)
Units
GBW Gain Bandwidth Product
CL = 20 pF, RL = 10 k to V+/2
22 MHz
G
M
Gain Margin
CL = 20 pF, RL = 10 k to V+/2
12 dB
Φ
M
Phase Margin
CL = 20 pF, RL = 10 k to V+/2
65 deg
R
IN
Input Resistance Differential Mode 38
k
Common Mode 151
M
THD Total Harmonic Distortion AV = 1, fO = 1 kHz, Amplitude = 1V 0.001
%
e
n
Input-Referred Voltage Noise f = 1 kHz, VCM = 4.5V
2.9 nV/
f = 1 kHz, VCM = 0.5V
2.9
0.1 Hz to 10 Hz 75 nV
PP
i
n
Input-Referred Current Noise f = 1 kHz, VCM = 4.5V
1.1 pA/
f = 1 kHz, VCM = 0.5V
2.2
Note 1: Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is intended to be functional, but specific performance is not guaranteed. For guaranteed specifications and the test conditions, see the Electrical Characteristics Tables.
Note 2: Human Body Model, applicable std. MIL-STD-883, Method 3015.7. Machine Model, applicable std. JESD22-A115-A (ESD MM std. of JEDEC) Field­Induced Charge-Device Model, applicable std. JESD22-C101-C (ESD FICDM std. of JEDEC).
Note 3: The maximum power dissipation is a function of T
J(MAX)
, θJA, and TA. The maximum allowable power dissipation at any ambient temperature is
PD = (T
J(MAX)
- TA)/ θJA. All numbers apply for packages soldered directly onto a PC board.
Note 4: Electrical Table values apply only for factory testing conditions at the temperature indicated. Factory testing conditions result in very limited self-heating of the device such that TJ = TA. No guarantee of parametric performance is indicated in the electrical tables under conditions of internal self-heating where TJ > TA. Absolute maximum Ratings indicate junction temperature limits beyond which the device maybe permanently degraded, either mechanically or electrically.
Note 5: Typical values represent the most likely parametric norm as determined at the time of characterization. Actual typical values may vary over time and will also depend on the application and configuration. The typical values are not tested and are not guaranteed on shipped production material.
Note 6: All limits are guaranteed by testing, statistical analysis or design.
Note 7: Ambient production test is performed at 25°C with a variance of ±3°C.
Connection Diagram
8-Pin SOIC
30015003
Top View
Ordering Information
Package Part Number Package Marking Transport Media NSC Drawing
8-Pin SOIC
LMP7732MA
LMP7732MA
95 units/Rails
M08A
LMP7732MAX 2.5k Units Tape and Reel
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LMP7732
Typical Performance Characteristics Unless otherwise noted: T
A
= 25°C, RL > 10 k, VCM = VS/2.
Offset Voltage Distribution
30015071
TCVOS Distribution
30015076
Offset Voltage Distribution
30015073
TCVOS Distribution
30015074
Offset Voltage Distribution
30015070
TCVOS Distribution
30015077
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LMP7732
Offset Voltage Distribution
30015072
TCVOS Distribution
30015075
Offset Voltage vs. Temperature
30015082
Offset Voltage vs. Temperature
30015083
PSRR vs. Frequency
30015029
CMRR vs. Frequency
30015062
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LMP7732
Offset Voltage vs. Supply Voltage
30015053
Offset Voltage vs. V
CM
30015054
Offset Voltage vs. V
CM
30015055
Offset Voltage vs. V
CM
30015056
Input Offset Voltage Time Drift
30015080
Slew Rate vs. Supply Voltage
30015020
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LMP7732
Input Voltage Noise vs. Frequency
30015063
Input Current Noise vs. Frequency
30015064
Time Domain Voltage Noise
30015067
Time Domain Voltage Noise
30015065
Time Domain Voltage Noise
30015066
Output Voltage vs. Output Current
30015057
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LMP7732
Input Bias Current vs. V
CM
30015025
Input Bias Current vs. V
CM
30015026
Input Bias Current vs. V
CM
30015027
Open Loop Frequency Response Over Temperature
30015018
Open Loop Frequency Response
30015019
Open Loop Frequency Response
30015028
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LMP7732
THD+N vs. Frequency
30015085
THD+N vs. Output Voltage
30015069
Large Signal Step Response
30015022
Small Signal Step Response
30015021
Large Signal Step Response
30015024
Small Signal Step Response
30015023
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LMP7732
Supply Current vs. Supply Voltage
30015081
Output Swing High vs. Supply Voltage
30015058
Output Swing Low vs. Supply Voltage
30015059
Sinking Current vs, Supply Voltage
30015060
Sourcing Current vs. Supply Voltage
30015061
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LMP7732
Application Notes
LMP7732
The LMP7732 is a dual low noise, low offset voltage, rail-to­rail input and output, low voltage precision amplifier.
The low input voltage noise of only 2.9 nV/
with a 1/f cor­ner at 3 Hz makes the LMP7732 ideal for sensor applications where DC accuracy is of importance.
The LMP7732 has very low guaranteed offset voltage of only ±40 µV. This low offset voltage along with the very low input voltage noise allows higher signal integrity and higher signal to noise ratios since the error contribution by the amplifier is at a minimum.
The LMP7732 has high gain bandwidth of 22 MHz. This wide bandwidth enables the use of the amplifier at higher gain set­tings while retaining ample usable bandwidth for the applica­tion. This is particularly beneficial when system designers need to use sensors with very limited output voltage range as it allows larger gains in one stage which in turn increases sig­nal to noise ratio.
The LMP7732 has a proprietary input bias cancellation cir­cuitry on the input stages. This allows the LMP7732 to have only about 1.5 nA bias current with a bipolar input stage. This low input bias current, paired with the inherent lower input voltage noise of bipolar input stages makes the LMP7732 an excellent choice for precision applications. The combination of low input bias current, low input offset voltage, and low input voltage noise enables the user to achieve unprecedented ac­curacy and higher signal integrity.
National Semiconductor is heavily committed to precision amplifiers and the market segment they serve. Technical sup­port and extensive characterization data is available for sen­sitive applications or applications with a constrained error budget.
The LMP7732 comes in the 8-pin SOIC package. This small package is an ideal solution for area constrained PC boards and portable electronics.
INPUT BIAS CURRENT CANCELLATION
The LMP7732 has proprietary input bias current cancellation circuitry on its input stage.
The LMP7732 has rail-to-rail input. This is achieved by having a p-input and n-input stage in parallel. Figure 1 only shows
one of the input stages as the circuitry is symmetrical for both stages.
Figure 1 shows that as the common mode voltage gets closer to one of the extreme ends, current I1 significantly increases. This increased current shows as an increase in voltage drop across resistor R1 equal to I1*R1 on IN+ of the amplifier. This voltage contributes to the offset voltage of the amplifier. When common mode voltage is in the mid-range, the transistors are operating in the linear region and I1 is significantly small. The voltage drop due to I1 across R1 can be ignored as it is orders of magnitude smaller than the amplifier's input offset voltage. As the common mode voltage gets closer to one of the rails, the offset voltage generated due to I1 increases and becomes comparable to the amplifiers offset voltage.
30015006
FIGURE 1. Input Bias Current Cancellation
INPUT VOLTAGE NOISE MEASUREMENT
The LMP7732 has very low input voltage noise. The peak-to­peak input voltage noise of the LMP7732 can be measured using the test circuit shown in Figure 2
30015079
FIGURE 2. 0.1 Hz to 10 Hz Noise Test Circuit
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LMP7732
The frequency response of this noise test circuit at the 0.1 Hz corner is defined by only one zero. The test time for the
0.1 Hz to 10 Hz noise measurement using this configuration should not exceed 10 seconds, as this time limit acts as an additional zero to reduce or eliminate the contributions of noise from frequencies below 0.1 Hz.
Figure 3 shows typical peak-to-peak noise for the LMP7732 measured with the circuit in Figure 2.
30015066
FIGURE 3. 0.1 Hz to 10 Hz Input Voltage Noise
Measuring the very low peak-to-peak noise performance of the LMP7732, requires special testing attention. In order to achieve accurate results, the device should be warmed up for at least five minutes. This is so that the input offset voltage of the op amp settles to a value. During this warm up period, the offset can typically change by a few µV because the chip temperature increases by about 30°C. If the 10 seconds of the measurement is selected to include this warm up time, some of this temperature change might show up as the mea­sured noise.Figure 4 shows the start-up drift of five typical LMP7732 units.
30015080
FIGURE 4. Start-Up Input Offset Voltage Drift
During the peak-to-peak noise measurement, the LMP7732 must be shielded. This prevents offset variations due to air­flow. Offset can vary by a few nV due to this airflow and that can invalidate measurements of input voltage noise with a magnitude which is in the same range. For similar reasons, sudden motions must also be restricted in the vicinity of the test area. The feed-through which results from this motion could increase the observed noise value which in turn would invalidate the measurement.
DIODES BETWEEN THE INPUTS
The LMP7732 has a set of anti-parallel diodes between their input pins, as shown in Figure 5. These diodes are present to protect the input stage of the amplifiers. At the same time, they limit the amount of differential input voltage that is al­lowed on the input pins. A differential signal larger than the voltage needed to turn on the diodes might cause damage to the diodes. The differential voltage between the input pins should be limited to ±3 diode drops or the input current needs to be limited to ±20 mA.
30015004
FIGURE 5. Anti-Parallel Diodes between Inputs
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LMP7732
DRIVING AN ADC
Analog to Digital Converters, ADCs, usually have a sampling capacitor on their input. When the ADC's input is directly con­nected to the output of the amplifier a charging current flows from the amplifier to the ADC. This charging current causes a momentary glitch that can take some time to settle. There are different ways to minimize this effect. One way is to slow down the sampling rate. This method gives the amplifier suf­ficient time to stabilize its output. Another way to minimize the glitch, caused by the switch capacitor, is to have an external capacitor connected to the input of the ADC. This capacitor is chosen so that its value is much larger than the internal switching capacitor and it will hence provide the charge need­ed to quickly and smoothly charge the ADC's sampling ca­pacitor. Since this large capacitor will be loading the output of the amplifier as well, an isolation resistor is needed between the output of the amplifier and this capacitor. The isolation resistor, R
ISO
, separates the additional load capacitance from the output of the amplifier and will also form a low-pass filter and can be designed to provide noise reduction as well as anti-aliasing. The draw back of having R
ISO
is that it reduces
signal swing since there is some voltage drop across it. Figure 6 (a) shows the ADC directly connected to the ampli-
fier. To minimize the glitch in this setting, a slower sample rate needs to be used. Figure 6 (b) shows R
ISO
and an external
capacitor used to minimize the glitch.
30015005
FIGURE 6. Driving An ADC
THERMOPILE AMPLIFIER
Thermopile Sensors
Thermopiles are arrays of interconnected thermocouples which can detect surface temperature of an object through radiation rather than direct contact. The hot and cold junctions of the thermocouples are thermally isolated. The hot junctions are exposed to IR radiation emitted from the measurement surface and the cold junctions are connected to a heat sink. The incident IR changes the temperature of the hot junctions of the thermopile and produces an output voltage proportional to this change.
The hot junction of the thermopile is covered with a highly emissive coating. The IR radiation incident to this highly emis­sive material changes the temperature of this coating. The temperature change is converted to a voltage by the ther­mopile. Emissivity represents the radiation or absorption ef­ficiency of a material relative to a black body. An ideal black body has an emissivity of 1.0. Excluding shiny metals, most objects have emissivities above 0.85. As a practical matter, shiny metals are not good candidates for IR sensing because of their low emissivity. The low emissivity means that the ma­terial is highly reflective. Reflective materials often “reflect” the surrounding environment's temperature rather than their own heat radiation. This makes them not suitable for ther­mopile applications.
The output voltage of a thermopile is related to temperature and emissivity by the following formula:
Where: V
OUT
: Output voltage of the thermopile
K : Proportionality constant
ε
OBJ
: Emissivity of object being measured
T
OBJ
: Temperature of object being measured
δ : Correction factor. This is needed since thermopile filters do not allow all wavelengths to enter the sensor
εTP: Emissivity of the thermopile
TTP: Temperature of the thermopile As mentioned above, the IR radiation generates a static volt-
age across the pyroelectric material. If the illumination is constant, the signal level detection declines. This is why the radiation needs to be periodically refreshed. This task is usu­ally achieved by the means of a mechanical chopper in front of the detector.
Thermopiles offer much faster response time compared to other temperature measurement devices. Packaged thermis­tors and thermocouples have response times that can range up to a few seconds, where as packaged thermopiles can easily achieve response times in the order of tens of millisec­onds. Thermopiles also provide superior thermal isolation compared to their contact temperature measurement coun­terparts. Physical contact disturbs the systems temperature and also creates temperature gradients.
Figure 7 shows a simplified schematic of a thermopile. The cold junctions are connected to a heat sink, and the absorber material covers the hot junction. The output voltage resulting from temperature difference between the two junctions is measured at the two ends of the array of thermocouples. As is evident in Figure 7, increasing the number of thermocou­ples in a thermopile increases the output voltage range. This also increases the active area of the thermopile sensor.
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LMP7732
30015007
FIGURE 7. Thermopile
Thermopiles have very wide temperature ranges of -100°C to 1000°C
When choosing a thermopile for a certain application, one must pay attention to several parameters. Some of these pa­rameters are discussed below:
Thermopiles' sensitivity, or responsivity, is determined by the ratio of output voltage to the absorbed input signal power and is usually specified in V/W. Typical sensitivity of thermopiles ranges from 10s of V/W to about 100 V/W. Generally, higher values of sensitivity are desirable. Sensitivity is dependent on the absorber's area and number of thermocouples used in the sensor. Sensitivity is often represented by S where:
S = V
OUT/PIN
The sensitivity of a thermopile changes with change in tem­perature. This change is usually specified as the Temperature Coefficient, TC, of sensitivity. Lower numbers are desired for this parameter.
Resistance of the thermopile is usually specified in the datasheet. This is the impedance which will be seen by the input of the amplifier used to process the thermopile's output signal. Typical values for thermopile resistance, RTP, range from 10s of kilo-ohms to about 100 k. This resistance is also a function of temperature. The temperature coefficient of the resistance is usually specified in a thermopile's datasheet. As with any other parameter, minimum variation with tempera­ture is desired.
The dominant noise source for a thermopile is its resistance. Noise spectral density of a resistor is calculated by:
Where k is the Boltzman constant and T is absolute temper­ature. Unit of noise spectral density is: V/
For the thermopile sensor, this noise is usually represented by V
NOISE
where:
Typical values for this voltage noise are in the order of a few tens of nV/ .
The Noise Equivalent Power, NEP, is often used to specify the minimum detectable signal level per square root band-
width. A smaller NEP is desired, however NEP is dependent on the thermopile active area, AD. For a thermopile:
And
As it is shown above, one cannot just compare the NEP of two thermopiles without considering the corresponding active areas.
A better way to compare thermopiles is to look at their specific detectivity, D*. Specific detectivity includes both the device noise and its sensitivity. It is normalized with respect to the detector's active area and also noise bandwidth. D* is given by:
Unit of D* is cm / W. Typical values for specific detectivity range from 108 to 3*108 cm / W.
After receiving radiation, the thermopile takes some time be­fore it comes to thermal equilibrium. The time it takes for the sensor to achieve this equilibrium is called response time or time constant of the sensor. Clearly, lower time constants are very desirable.
Precision Amplifier
Since the output of thermopiles are usually very small and at most in the order of only a few millivolts, the first part of the signal conditioning path should involve amplification. In choosing an amplifier for this purpose, a few different sensor characteristics and the way they interface with the amplifier should be considered. These are:
Sensor's Impedance and Opamp's Input Bias Current The input bias current causes a voltage drop across the sen-
sor and the amount of this voltage is equal to the sensor's impedance multiplied by the magnitude of bias current. The higher the sensor's input impedance, the more accentuated the effect of amplifier's input bias current will be. For very high impedance sensors, it is imperative that opamps with very low input bias currents be used. Thermopiles have input impedances in the range of 100 k, so input bias current is not as critical as in some other applications.
Sensor's output voltage range: The output signal of the sensor is fed into the opamp where
it will be amplified or otherwise conditioned, (e.g. level shifted, buffered.) It is important to pay attention to different parame­ters of this output signal.
One important aspect is the lowest expected level of the sensor's output and compare that with different parameters contributing to the amplifier's total input noise. If the sensor's output level is in the same order of magnitude or smaller than the opamp's total input noise, then signal integrity at the opamp's output and the ADC's input will be compromised.
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LMP7732
30015078
FIGURE 8. Thermopile Amplifier
Figure 8 shows the LMP7732 used as a thermopile amplifier. The LMP7732 is a great choice for use with thermopile sen­sors. The LMP7732 provides unprecedented accuracy and precision because of its very low input voltage noise and the very low 1/f corner frequency. The 1/f noise is one of the main sources of error in DC operating mode. Since thermopiles and most other sensors operate on DC signals, signal integrity at the DC level is very important. The LMP7732 also has very low offset voltage and offset voltage drift which greatly re­duces the effects of input offset voltage of the amplifier on the thermopile signal. The thermopile used in this circuit is TPS332 from PerkinElmer Optoelectronics, PKI. This ther­mopile has an internal resistance, RTP, of 75 kΩ. The output voltage of the thermopile is represented with a DC voltage source. The TPS332 has a thermistor integrated in the pack­age. The thermistor is used to measure the ambient temper­ature of the thermopile at the time of measurement. The thermistor's resistance at room temperature is 30 k. More information about this thermopile and other sensors from PKI can be found on http://www.perkinelmer.com/
The circuit in Figure 8 shows how the LMP7732 is connected to the thermopile. This circuit is comprised of two LMP7732 amplifiers, the LM4140A-2.5 which is a precision voltage ref­erence, the ADC122S021 which is a two channel Analog to Digital converter, and the thermopile sensor. Note that the two amplifiers used in this circuit are numbered for ease of refer-
ence. The LMP7732 amplifiers are referred to as amplifier 1 and amplifier 2 per Figure 8.
In Figure 8the LM4140A is providing a precision voltage ref­erence of 2.5V. This reference voltage is applied to the ther­mistor via the 30 k resistor. The thermistor's resistance is converted to a voltage using this set up. This voltage is fed into the ADC's channel one. The ADC uses this voltage and the thermistor's look up table to convert this voltage to tem­perature. The 2.5V reference is also fed into amplifier 1, which is configured as a buffer. This LMP7732 transfers the 2.5V signal to both inputs of amplifier 2. This means the 2.5V will show up on the output of amplifier 2. Having an output level that is mid-supply is important since the thermopile sensor has a bipolar output signal and this way the amplifier can ac­curately gain the thermopile voltage, whether its polarity is positive or negative. It is also important because the output signal of amplifier 2 is only positive. ADCs can only handle positive signals on their inputs. Amplifier 2 is used to gain and filter the thermopile signal. The low pass filter ensures that AC noise will not be gained up and, as a result, the output signal will be cleaner. The output of amplifier 2 is fed into the ADC's channel 0. The ADC uses the ambient temperature, which was calculated using the voltage on Channel 1 and the thermistor's look up table, along with the thermopiles' gained output voltage available on channel 0 and the thermopile's look up table to determine the object's temperature.
www.national.com 18
LMP7732
Physical Dimensions inches (millimeters) unless otherwise noted
8-Pin SOIC
NS Package Number M08A
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LMP7732
Notes
LMP7732 Low Noise, Precision, RRIO Amplifier
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