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Model
IM-IT-IRP3
IM-IT-IRP5
IM-ITC-IRP0
Supply Voltage
12~24V
6~24V 0.1W
Temperature Measurement Accuracy [1]
±1℃/ 1%
Repeatability [2]
±0.5℃/0.5%
Maximum Temperature Range
【See Selection Table for Details】
-40~600℃
-40~1200℃
0~500℃
Minimum Spot Diameter
7mm
Optical Resolution
(10:1, 90% Energy)
Temperature Coefficient [3]
0.1K
Spectral Range
8~14um
Analog Temperature Resolution [4]
0.1℃/0.1%
Digital Temperature Resolution [5]
0.01℃
No Digital Output
Response Time (95%)
20~5000ms (Adjustable)
150ms (Fixed)
Emissivity
0.1~1.5 (Adjustable)
0.95 (Fixed)
Transmittance
1.0 (Fixed)
Output Signal Processing
Average, Median, Quantile, Peak Hold, Valley Hold
Average (Fixed)
Supporting Software
SensIRTS
None
Output Mode
Digital + Analog Output Simultaneously
Analog Voltage Output Only
Analog Output Specification
0-10V
0~5V
Analog Output Load
Max for current output: 500Ω
Min for voltage output: 100KΩ
Voltage Output (Min): 30KΩ
Stabilization Time
10min
Digital Output Mode
RS485/Modbus
Analog Output Only
Alarm Range Setting
Digital Setting
Alarm Output
Digital Output
Cable Specification
6 Wires
3 Wires
Cable Length
2m (Default)
1m (Default)
Operating Temperature Range
-20~85℃
Storage Temperature Range
-40~85℃
Relative Humidity
10-95% Non-condensing
Vibration Resistance
10~150Hz, 1.5mm Double Amplitude, 2 Hours per XYZ Axis
Shock Resistance
50G, 10 Times per Direction on XYZ Axes
Mounting Dimension
M18×1
φ12×85
Housing Material
SUS 304
Protection Class
IP65
Weight
75g
70g
Mounting Bracket
Standard L-shaped Mounting Bracket and M18 Nut
Featured Function
This model allows users to customize the temperature range of analog output within the specified model specifications. For example, when selecting a model with 0-300℃, users can define the analog output range as 20-120℃ in SensIRTS software, and then the 0-20mA output will correspond to 20-120℃, thus improving the resolution of analog output, which is beneficial for the sensor to play a greater role within the range specified by the user.
Remarks
[1][2] Take the larger value, measured when the ambient temperature is 23±5℃ and the target is a standard blackbody at 100℃
[3] Calculated by measuring a standard blackbody at 100℃ at ambient temperatures of 40℃ and 80℃ respectively
[4] Resolution of analog output
[5] Digital resolution obtained by using DagaSensIRTS software or digital communication.
Temperature measurement range code
Code
T range(℃)
A
-40
F
45
L
150
R
400
B
-20
G
64
M
180
S
500
C
0
H
80
N
200
T
600
D
16
J
100
P
250
U
800
E
25
K
120
Q
300
V
1000
For example: AR indicates that the temperature measurement range is: -40 to 400℃. BV indicates that the temperature measurement range is: -20 to 1000℃
Note: The temperature measurement range is not an arbitrary combination. The method of taking values is shown in the selection reference table.
Temperature measurement range
Output
Configuration information
IM-IT-IRP3-AJ
-40~100℃
RS485&0~10V
2m straight power cord
IM-IT-IRP3-CJ
0~100℃
IM-IT-IRP3-AN
-40~200℃
IM-IT-IRP3-CN
0~200℃
IM-IT-IRP3-AQ
-40~300℃
IM-IT-IRP3-CQ
0~300℃
IM-IT-IRP3-AS
-40~500℃
IM-IT-IRP3-CS
IM-IT-IRP3-AT
IM-IT-IRP3-CT
0~600℃
IM-IT-IRP5-AI
-40~800℃
IM-IT-IRP5-CI
0~800℃
IM-IT-IRP5-AV
-40~1000℃
IM-IT-IRP5-CV
0~1000℃
IM-IT-IRP5-AW
IM-IT-IRP5-CW
0~1200℃
IM-ITC-IRP0-CJ
1 m power cord
IM-ITC-IRP0-CN
IM-ITC-IRP0-CQ
IM-ITC-IRP0-CR
0~400℃
IM-ITC-IRP0-CS
Basic composition
The structure of the IR pyrometer is designed around the logic of "capturing radiation - converting signals - processing and calculating - outputting results", and its core components include four major modules:
Working principle
The core operation of an infrared pyrometer follows the fundamental law of thermal radiation: any object with a temperature above absolute zero (-273.15℃) will continuously radiate infrared rays (an invisible light) outward, and the intensity and wavelength distribution of the radiation are directly related to the temperature of the object.
According to Planck's law of radiation, the spectral distribution of an object's infrared radiation varies with temperature. The higher the temperature, the shorter the peak wavelength of the radiation and the stronger the total energy of the radiation. According to the Stefan-Boltzmann law, the total infrared radiation power per unit area of an object is directly proportional to the fourth power of the thermodynamic temperature, which is the key basis for the conversion between temperature and radiation energy. The infrared pyrometer captures the infrared radiation of the object being measured through an optical system. The infrared detector converts the radiation signal into an electrical signal, which is then amplified, filtered and compensated by the signal processing circuit. Finally, it is converted into the surface temperature of the object according to the preset algorithm and the reading is output through the display unit. Some models can also synchronously transmit the temperature signal to the control system.
The emissivity of an object (a parameter characterizing the object's ability to radiate infrared rays, with a value ranging from 0 to 1) directly affects the measurement accuracy. Therefore, most infrared pyrometers have an adjustable emissivity function and can be calibrated according to the characteristics of the material being measured (such as metals and non-metals) to ensure accurate results.
The reference table for the emissivity of common substances is as follows:
Matter
Black fabric
0.98
Water
0.92~0.96
Sand
0.9
Alumina
0.2~0.3
Human skin
Ice
0.96~0.98
Fur
0.75~0.8
Chromium oxide
0.81
Asphalt
0.9~0.98
Snow
0.83
Carbon powder
0.96
Copper oxide
0.78
Cement
Glass
0.9~0.95
Black paint
0.97
Iron oxide
0.78~0.82
Concrete
0.94
Ceramic
0.9~0.94
Rubber
Zinc oxide
0.11~0.28
Soil
Gypsum
0.8~0.9
Plastic
0.85~0.95
copper
0.1~0.3
Marble
Lime
0.89~0.91
Matte paint
0.8~0.95
Stainless steel
0.45
Wood
Optical fiber
Lithium electrode sheet
Carbon steel
0.69
paper
0.7~0.94
Red brick
0.93~0.95
Graphite
0.7~0.8
Lead
0.6
Note: The emissivity data in the above table is for reference only. The actual emissivity of an object is affected by its surface shape and measurement method. Factors such as frosted surface, polished surface, painted surface, measurement Angle, and target temperature can all influence the actual emissivity.
Therefore, during the use of infrared temperature sensors, the emissivity of objects can be determined through the following methods. For objects with high reflectivity, first measure the surface temperature of the object using a direct-reading thermocouple, then align the infrared temperature sensor with the same area and modify the sensor's emissivity until the temperature is the same as the measured value. At this point, the emissivity can be used as the emissivity of the object. For objects with too low emissivity, it is necessary to use blackbody tape to indirectly measure the surface temperature of the object. Apply blackbody adhesive tape to the surface of a low-emissivity object, and then set the emissivity to 0.95 to measure its temperature.
Note: Even with the above Settings, there may still be errors between the sensor measurement values and the actual object temperature (as the emissivity of some objects changes at different temperatures). Therefore, the high measurement accuracy can be improved by on-site secondary calibration. The digital sensor is equipped with parameter Settings for user secondary calibration. Through these parameters, the secondary calibration of the sensor can be conveniently achieved.
Indicator
IM-IT-IRP3/5
Core count and specification
6-core AWG26
Min. bending radius
25mm (Fixed installation);50mm (Mobile installation)
Lifespan
Bend 4 million times
Temperature range
-20 to 85℃ (Fixed installation);-5 to 80℃ (Mobile installation)
Types of connectors
Straight head connector (default);90° elbow connector (optional)
Standard length of the wiring harness
2m
Definition of Wiring Harness
Brown: Power supply positive (+)
White: Power ground (-)
Blue: RS485A+
Black: RS485B-
Gray: Simulated output location (-)
Pink: Analog output positive (+)
Brown :6~24V power supply positive
White: Power ground
Pink: Analog output
This protocol defines the communication rules and contents between infrared temperature sensors and upper computers as well as PLCS. Based on RS485 communication, the Modbus-RTU protocol has been implemented, which is well compatible with the two mainstream upper-level controllers, PC and PLC. Through this protocol, users can conveniently set multiple parameters of the sensor, read data and store it, which is convenient for later analysis.
Communication parameter Settings: The default communication parameters at the factory are as follows: Baud rate :57600, no parity,8 data bits, and 1 stop bit.
Content of Modbus-RTU protocol: The communication mode of this protocol is question-and-answer mode. The upper computer is the active controller (Master), and the sensor is the passive responder (Slave). In the question-and-answer mode, the active controller sends the corresponding request according to the protocol content, and then the passive responder with a specified ID responds to the request, executes the command, and feeds back the data or execution result.
NOTE:For more details about the agreement, please refer to the relevant content in the user manual section.
Some models of sensors support RS485 communication output function, and parameters can be easily managed and set through the corresponding software.
Comparison of the measured area and the size of the light spot
To ensure accurate measurement, it is recommended that the size of the object to be measured be 1.5 futian larger than the size of the light spot. The measured temperature is the comprehensive temperature of the measured area. If the measured light spot is larger than the actual object, the measured temperature will include part of the background temperature, causing the measured value to shift towards the background temperature.
Confirmation of installation angles
To ensure accurate measurement, the Angle between the sensor's axis and the normal of the object being measured must be less than 45°. Due to the different measurement angles, the emissivity of the object being measured varies in a certain direction. Therefore, if the installation Angle changes, the emissivity needs to be reset.
Measurement of large-area high-temperature heat sources
When measuring large-area high-temperature heat sources, due to the scorching effect of the high-temperature heat source on the sensor, the temperature of the sensor will rise or change significantly and continuously, thereby affecting the measurement accuracy. At this time, a orifice plate can be installed in front of the sensor to block the heat source, which can improve the measurement accuracy and stability.
Isolated USB-RS485 adapter:An RS485 port can be extended on a PC
Simple display instrument:Can be used to display the measured temperature
Black body adhesive tape:Can be used for temperature measurement or emissivity assessment of low-emissivity objects. The emissivity of the blackbody adhesive tape is 0.95
Laser collimator:Can be used for IRTSM series of infrared pyrometer auxiliary alignment of the measurement
Universal mounting frame:Be used for installing IRTSM series high-temperature meters and has the function of universal adjustment
Dust cover:Can be used in IRTSM series sensors to prevent dust and oil mist from contaminating the lens and improve sensor durability in harsh conditions.
Condenser hood:Infrared pyrometer measurement kit
USB direct reading thermocouple:Can be used to contact surface temperature, measuring the emissivity of auxiliary measuring objects.
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