This user's guide describes the function and operation of the TMP006, a non-contact infrared (IR) sensor
with a digital interface. This document discusses the most important application-related design
considerations to achieve optimal performance when using the TMP006 for surface temperature
measurements.
The following list summarizes many of the terms and abbreviations used in this document.
•PCB: Printed circuit board; specifically refers to the printed circuit board that the TMP006 is mounted
on.
•IR: Infrared, or radiation that occurs in the infrared wavelengths (0.7 μm to 1000 μm). The TMP006
uses IR wavelengths from 4 μm to 8 μm.
•IR sensor, Sensor: The IR sensor within the TMP006 integrated circuit device.
•Target object, Target: The object for which the TMP006 measures the temperature.
1.2If You Need Assistance
If you have questions about the TMP006, join the discussion with the Linear Amplifiers Temperature
Sensors Applications Team in the e2e™ forum at e2e.ti.com. Include TMP006 as the subject heading of
your posting.
1.3Information About Cautions and Warnings
This document contains caution statements.
This is an example of a caution statement. A caution statement describes a
situation that could potentially damage your software or equipment.
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CAUTION
The information in a caution or a warning is provided for your protection. Please read each caution and
warning carefully.
1.4FCC Warning
This equipment is intended for use in a laboratory test environment only. It generates, uses, and can
radiate radio frequency energy and has not been tested for compliance with the limits of computing
devices pursuant to subpart J of part 15 of FCC rules, which are designed to provide reasonable
protection against radio frequency interference. Operation of this equipment in other environments may
cause interference with radio communications, in which case the user at his own expense is required to
take whatever measures may be required to correct this interference.
Figure 1 shows an example of the TMP006 in a typical target object surface temperature measurement
setup.
System Overview
NOTE: Drawing not to scale; for illustration purposes only. The TMP006 field of view is much wider than shown here.
Figure 1. TMP006 in a Target Object Temperature Measurement Setup
The TMP006 must be mounted on a printed circuit board (PCB). Section 4 reviews the details of the PCB
construction.
CAUTION
Many of the components mounted on a PCB (including the TMP006) are
susceptible to damage by electrostatic discharge (ESD). Customers are
advised to observe proper ESD handling precautions when handling the TMP
as configured on a PCB, including the use of a grounded wrist strap at an
approved ESD workstation.
When measuring the temperature of an object using the TMP006, there are several fundamental
measurement constraints that must be followed to ensure the accuracy of the object temperature
calculation. The two primary constraints are:
•The surface emissivity of the target object; and
•The placement of the TMP006, relative to the size of the target.
The next two subsections examine these constraints in particular.
3.1Target Object Emissivity Guidelines
The emissivity of an object is defined as the ability of an object surface to radiate energy relative to an
ideal emitter. An ideal emitter, also called a black body, has an emissivity value of 1. When using the
TMP006 for target object surface temperature calculations, it is essential that the surface of the target
object be able to emit sufficient IR radiation to be accurately detected by the IR sensor in the TMP006.
Targets with very low emissivity values emit less IR radiation, and therefore produce smaller signals,
which are harder for the TMP006 to capture and measure. Polished and shiny metal objects have surface
emissivity values that are typically too low for use with the TMP006.
To measure the surface temperature of an object with a very low emissivity, it can be painted with
lampblack paint which has an emissivity of 0.96.
As a design guideline, the TMP006 should only be used to calculate the surface temperature of target
objects with emissivity values greater than 0.7, and preferably greater than 0.9. The emissivity values of
common objects are listed in Table 1.
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Table 1. Emissivity Values for Common Objects
Object or MaterialEmissivityObject or MaterialEmissivity
Aluminum, commercial sheet0.09Nickel, electroplated0.03
Aluminum, polished0.039 to 0.057Porcelain, glazed0.92
Aluminum, anodized0.77Paper0.93
Brass, dull plate0.22Paint0.8-0.96
Brass, polished0.03Plaster0.92
Brick, red rough0.90Plastics0.91
Cast Iron, turned and heated0.6 to 0.7Sand0.76
Chromium, polished0.08 to 0.36Sawdust0.75
Concrete0.85Silver, polished0.02 to 0.03
Cotton, cloth0.77Steel, mild0.2 to 0.32
Copper, polished0.08 to 0.036Steel, oxidized0.79
Glass0.92Steel, polished0.07
Gold, pure and polished0.018 to 0.035Steel, galvanized old0.88
Granite0.45Steel, galvanized new0.23
Gypsum0.85Stainless steel, weathered0.85
Ice0.97Stainless steel, polished0.075
Iron, polished0.14 to 0.38Tile0.97
Iron, plate rusted red0.61Water0.95
Lampblack paint0.96Wood, oak0.91
Marble, white0.95Wrought iron0.94
The TMP006 can accurately detect signals in almost the entire 180° field of view of the sensor. The final
calculated target object temperature is an integration of all of the signals present in the sensor field of
view. Therefore, the ability of the TMP006 to accurately calculate the temperature of a target depends on
ability of the IR sensor to capture the majority of its signal from the target. This capture effectiveness, in
turn, depends on two factors: the angle of incidence and the distance of the TMP006 from the target.
Figure 2 illustrates the dependence of the TMP006 on the angle of incidence compared to the IR signal
absorption. For this test, the intensity of an input signal was held constant and was moved throughout the
sensor field of view. This figure shows that the majority of the received signal comes from IR sources
located at 0° angles of incidence.
TMP006 Object Temperature Measurement Setup
Figure 2. Percentage of IR Signal Absorbed by Sensor versus Angle of Incidence
As a design guideline, place the TMP006 directly underneath the target object with the surface of the
target parallel to the TMP006, so the angle of incidence between them is 0°.
The distance that the TMP006 should be placed from the target is largely dictated by the size of the target.
Smaller targets must be placed closer to the TMP006 to ensure that the majority of the IR signal captured
by the sensor is emitted from the target. A circular target should be placed at a distance less than one-half
of the radius of the target to ensure at least 90% of the IR signal that the sensor captures is from the
target.
As the sensor is moved away from the target, other objects or surfaces enter into the device field of view.
Because the final result is an integration of the entire field of view of the sensor, it is not possible to
determine which captured signals come from the target and which captued signals come from the other
objects (or surfaces).
As a design guideline, then, the target object should be placed at a distance no further than one-half of the
radius of the target from the TMP006.
Figure 3 shows how the percentage of the final IR signal captured by the TMP006 depends on the radius
of the target and its distance from the TMP006.
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4TMP006 Layout Guidelines
6
NOTE: Drawing not to scale; for illustration purposes only. The TMP006 field of view is much wider than shown here.
Figure 3. Relationship Between Target Object Size and Distance from the TMP006
The IR thermopile sensor in the TMP006 is as susceptible to conducted and radiant IR energy from below
the sensor on the PCB as it is to the IR energy from objects in its forward-looking field of view. When the
area of PCB below the TMP006 is at the same temperature as the die or substrate of the TMP006, heat is
not transferred between the IR sensor and the PCB. However, temperature changes on a closely-placed
target object or other events that lead to changes in system temperature can cause the PCB temperature
and the TMP006 temperature to drift apart from each other. This drift in temperatures can cause a heat
transfer between the IR sensor and the PCB to occur. Because of the small distance between the PCB
and the bottom of the sensor, this heat energy will be conducted (as opposed to radiated) through the thin
layer of air between the IR sensor and the PCB below it. This heat conduction causes offsets in the IR
sensor voltage readings and ultimately leads to temperature calculation errors. To prevent and minimize
these errors, the TMP006 layout must address three critical factors:
1. Match the thermal time constant of the PCB below the TMP006 IR sensor with the TMP006 sensor
itself.
2. Thermally isolate the TMP006 from the rest of the PCB and any heat sources on it.
3. Provide a stable thermal environment to reduce the noise in the measurement readings.
Guidelines for creating a PCB that has been used and tested extensively by Texas Instruments are shown
in Figure 4 through Figure 6. These PCB layout guidelines are based on a simplified two-layer design for
the TMP006 that has no significant performance reductions from the four-layer design used on the
TMP006EVM. For a more complete understanding of the TMP006 layout requirements as well as detailed
layout design guidelines used for the TMP006EVM, refer to the related document TMP006 Layout and
Assembly Guide (SBOU108), available for download from the TI website.
The bottom layer of the TMP006 two-layer PCB is shown in Figure 6.
Object Temperature Calculation
Figure 6. TMP006 Two-Layer PCB: Bottom Layer
5Object Temperature Calculation
Once the TMP006 has been installed in a system, measurements of the local temperature and object
voltage can be made with the TMP006 through the digital interface. Using these two measurements, the
target object temperature can be calculated. Section 5.1 presents the calculations required to solve for a
target object temperature. V
temperature (Register 1) registers in the TMP006, respectively.
are the readings from the object voltage (Register 0) and local
DIE
9
Page 10
S = S 1 + a (TT) + a
01 DIEREF2
-
2
(TT)
DIEREF
-
V= b + b (TT) + b
OS
01 DIEREF2
-
2
(TT)
DIEREF
-
?(V) = (V ) + c
OBJ
-
OS2
2
V(VV )
OBJOBJ
-
OS
T
DIE
4
+
?(V)
S
OBJ
(
(
T
OBJ
=
4
?(V)
OBJ
1 + a (TT) + a
1 DIEREF2
-
2
(TT)
DIEREF
-
Calibration Function =
Calibrating the System
5.1Equations for Calculating Target Object Temperatures
The target object temperature calculations consist of a series of equations that can be used to solve for
the target object temperature (T
sensor and how it changes over temperature:
Equation 1 also contains the primary calibration factor, S0, which is discussed more in Section 6.
Equation 2 describes an offset voltage that arises because of the slight self-heating of the TMP006,
caused by the non-zero thermal resistance of the package and the small operational power dissipation (1
mW) in the device:
Equation 3 models the Seebeck coefficients of the thermopile and how these coefficients change over
temperature.
Equation 4 relates the radiant transfer of IR energy between the target object and the TMP006 and the
conducted heat in the thermopile in the TMP006.
Solve the system of equations to calculate the temperature of the target object in Kelvins.
The terms used in these formulas are:
•V
•T
: Voltage in TMP006, Register 0
OBJ
: Temperature in TMP006, Register 1
DIE
•S0: Calibration factor (should be calibrated)
•a1: 1.75 × 10
•a2: –1.678 × 10
•T
: 298.15 K
REF
•b0: –2.94 × 10
•b1: –5.7 × 10
•b2: 4.63 × 10
–3
–5
–5
–7
–9
•c2: 13.4
) in Kelvins. Equation 1 represents the sensitivity of the thermopile
OBJ
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(1)
(2)
(3)
(4)
6Calibrating the System
The final step to calculate the temperature of the target object is to calibrate the system by calculating the
appropriate sensitivity factor, S0. The term S0is unique to a given system and can be determined with a
simple two-point calibration performed on one or several devices. S0is an accumulation of the
system-related signal reductions that can occur when using the TMP006/ This value is part of Equation 1
in the object temperature calculations. This series of equations (for the object temperature calculations)
are derived in a way that reduces all application-related factors to a single gain error term. Because the
errors only create a gain error, the S0term can be determined with a simple two-point calibration. The
primary contributors to S0are the field of view and emissivity of the target object (refer to Section 3 for
additional discussion of these two factors).
To determine S0, plot the Calibration Function as shown in Equation 2 versus T
the slope of a linear approximation of the plotted data.
In order to plot the Calibration Function versus T
must first be measured using an accurate temperature probe. The local die temperature measurement
should be taken from the TMP006 local temperature sensor (Register 1). Ideally, the two points used for
the linear slope-fit represent two extreme temperature points in the system. For example, the first
temperature measurement point could be taken with the main system in standby mode, and the second
temperature measured with the system running at full power.
Figure 7 shows a plot of the calibration function for several TMP006 devices tested in the same system.
The calibration functions for the TMP006 devices were plotted over many temperatures by accurately
controlling the local temperature and the object temperature using test equipment. Figure 7 shows that all
errors are only gain errors; device-to-device variation is limited, meaning that the calibration can be
performed on only a single device. This plot features many measurement points for each device; although
only two points are required for calibration, using more data points produces a more accurate curve fit.
OBJ
4
– T
Calibrating the System
4
, the actual temperature of the object (T
DIE
OBJ
)
Figure 7. Finding the Slope of the Calibration Function vs T
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