There are two main ways to measure temperature: one is the traditional contact measurement, and the other is non-contact measurement represented by infrared temperature measurement. Traditional temperature measurement not only has a slow response speed, but also requires contact with the object being measured. Infrared temperature measurement uses infrared
1. Working principle of infrared thermometer
All objects in nature with a temperature higher than absolute zero are constantly emitting infrared rays. The energy and wavelength distribution of infrared rays emitted by an object are closely related to its surface temperature. The radiation energy of an object is proportional to the fourth power of the temperature, and the relationship between its radiation energy density and the temperature of the object itself conforms to Planck's law. Therefore, we can determine the surface temperature of an object by measuring the amount of infrared energy radiated by the object. Slight temperature changes will cause obvious changes in radiation energy, so the sensitivity of using infrared radiation to measure temperature is very high. In addition to relying on temperature and wavelength, the radiance of an actual object is also related to factors such as the material properties and surface state of the object. As long as a radiation coefficient that changes with the material properties and surface state is introduced, the basic law of black bodies can be applied to actual objects. This radiation coefficient is the emissivity ε, or the specific emissivity, which is defined as the ratio of the radiation performance of an actual object to that of a black body at the same temperature. This coefficient indicates the degree of closeness between the thermal radiation of an actual object and the radiation of a black body, and its value is between 0 and 1.
The working principle of the infrared thermometer is shown in Figure 1: The infrared energy radiated by the object to be measured is transmitted to the infrared thermometer through the air.
The objective lens of the thermometer focuses infrared rays onto the infrared detector, which converts the radiation energy into electrical signals. The signals are amplified, shaped, and filtered by
2. System hardware design
This infrared temperature detection system is mainly composed of sensor A2PTMI, LM358 active filter circuit, AD conversion circuit, microprocessor, display circuit and other parts. Because the signal output by the sensor is 0-5V, which just meets the requirements of AD conversion, the amplifier circuit is omitted in this design, and only the sensor signal is filtered. In addition, this system also has a signal conversion circuit to output 4~20mA, 1~5V and other
2.1 Sensor A2PTMI principle and its application
PerkinElmer A2TPMI is a multi-purpose infrared thermopile sensor with dedicated signal processing circuit and ambient temperature compensation circuit integrated inside. This integrated infrared sensor module converts the thermal radiation of the target into analog voltage. The sensor has an optical system with a distance coefficient D:S=8:1. The infrared radiation in the air is received through the lens and then converted into a corresponding voltage signal, which is amplified by an 8-bit resolution programmable amplifier. According to the thermopile temperature measurement principle, the thermopile voltage may be positive or negative, depending on whether the target temperature is higher or lower than the ambient temperature of the A2TPMI. In order to enable negative voltage signals to be processed in a single power supply system, all internal signals are connected to the 1.255 V internal voltage reference (Vref) as a virtual analog ground signal. In order to adjust the bias voltage of the thermopile amplifier circuit, the amplifier has a programmable adjustment section that can generate a bias voltage with 8-bit resolution. In addition, the A2TPMI also integrates a
2.2 Filter circuit design
The A2TPMI amplifier uses chopper amplifier technology. Due to the characteristics of this technology, the output signals VTobj and VTamb contain about 10 mV peak, 250 kHz AC signals. These AC signals can be suppressed by an electronic low-pass filter circuit or similar software filtering. In high impedance load applications, rail to rail
The second type of filtering circuit is used in this design. Because the open-loop voltage gain and input impedance of the integrated operational amplifier are very high and the output impedance is low, the active filtering circuit has a certain voltage amplification and buffering effect, with good filtering effect, which improves the accuracy of the sensor signal.
2.3 AD conversion circuit
TLC2543 is a 12-bit switched capacitor successive approximation analog-to-digital
2.4 Characteristics of SOC-level microprocessor This system uses SOC-level STC series single-chip microcomputers, whose instruction codes are fully compatible with traditional 51 single-chip microcomputers and whose operating frequency can reach 48HZ. The microprocessor used in this design has 6 clock cycles, so its operating frequency is equivalent to the 96MHZ of ordinary 51 single-chip microcomputers, which provides speed guarantee for this system. In addition, the STC89C58RD selected in this design contains a 32K program storage area and an internal expansion of 32K data FLASH memory, so that this design can easily expand related functions, such as parameter memory function. This microprocessor also supports IAP and ISP, and does not require a dedicated programmer, and the program can be debugged through an ordinary serial port. Anti-interference is also one of the reasons for choosing this single-chip microcomputer. This design is mainly used for temperature monitoring of industrial equipment, so anti-interference is very important. [page]
3. System software design
The software design of infrared temperature detection system mainly includes the following main modules: initialization module, I/O port query module, AD conversion module, data processing module, data correction module, display driver module, etc. In addition, there is an interrupt program processing module: 0 external interrupt, which is mainly used for parameter setting.
The software design process is shown in Figure 3.
The whole program is written in C51. The initialization module is mainly used to initialize the alarm signals of each channel, set the parameters such as emissivity to the default value and display them. The main program continuously scans the 12-bit digital signal sent by the AD conversion module through the I/O port query module. The communication method of the SPI bus is adopted in this program, and the serial interface method saves a large number of IO ports. After the received digital signal is processed by the data processing module, the temperature value is obtained by the table lookup method. The temperature value is corrected by the data correction module and sent to the display module for display, and the data is transmitted to the host computer interface for display, thus completing the temperature measurement of one channel. During the operation of the program, the parameters such as emissivity and alarm value can be set at any time. When the function key is pressed, the 0 external interrupt of the single-chip microcomputer is triggered, and the parameter setting button is scanned in the interrupt program, and the result is stored. After each temperature measurement is completed, the system transmits the temperature value to the host computer through RS485 and displays it on the VB interface.
1 Experimental data processing and emissivity setting
2 Least squares fitting of experimental data
For a measurement system, its precision and accuracy are very important. Although this design uses 12-bit AD, which lays the foundation for the high precision of this design, due to
the inevitable errors of
In the best square approximation of a function, function f(x)∈C[a,b], if f(x) is only given on a set of discrete points {xi, i=0,1,…,m}, then we need to perform curve fitting on the experimental data {(xi,yi), i=0,1,…,m}, where yi= f(xi). If the function y="S" ((*)x) is required to fit the given data {(xi,yi), i=0,1,…,m}, then the error δi= S *(x)-yi. Let Φ 1(x), Φ2(x),…, Φn(x) be a family of linearly independent functions on C[a,b], and find a function S ((*)x in Φ =span{Φ1(x), Φ2(x),…, Φn(x)} to minimize the sum of squared errors. Because the amount of experimental data is large, in actual operations, we can use mathematical tools such as MATLAB to complete curve fitting by calling or writing related functions, and finally select appropriate results for output. [page]
4.2 Setting of emissivity ε
According to the principle of infrared temperature measurement, we should first determine the emissivity of the object being measured during testing. In higher temperature measurement applications, the emissivity ε of the object being measured should be actually measured, otherwise serious errors will occur. For power equipment, its emissivity is generally between 0.85-0.95. What is measured is the blackbody radiation temperature of the object being measured. In actual measurement applications, the blackbody radiation temperature TP needs to be converted to the actual temperature T. The conversion formula is: T=T Pε-¼
The emissivity determination method is as follows: First, select an object to be measured and determine the actual temperature T of the object to be measured (for example, 300K). Of course, other temperatures can also be selected. The temperature value can be measured by a thermal resistor or other temperature measuring equipment. Then, aim the temperature measurement system at the object to be measured and obtain a temperature value TP="T0". The set value of ε is obtained through the above formula; then the ε value is input into the system and tested again. By fine-tuning the ε value until T 0= T, the obtained ε value is the actual emissivity of the object. The actual emissivity ε of the same object to be measured is basically the same. If the material and shape of the object to be measured change, its emissivity will change, and its actual emissivity can be measured by the same method. This design has an emissivity setting and adjustment part, which can easily adjust the emissivity value. In this way, the same temperature measuring equipment can be used to adjust the emissivity to meet the temperature measurement requirements of various materials.
6. Conclusion
Non-contact infrared thermometers use infrared technology to quickly and easily measure the surface temperature of an object. Temperature readings can be quickly measured without mechanical contact with the object being measured. Just aim and read the temperature data on the display. Infrared thermometers are light, small, easy to use, and can reliably measure hot, dangerous or hard-to-reach objects without contaminating or damaging the object being measured. In addition, infrared thermometers can measure several readings per second, while contact thermometers take several seconds for each measurement. After experimental comparison, the error between this thermometer and the infrared thermometer produced by Fluke Corporation of the United States is within one degree, but this thermometer has a parameter setting function and is cheaper, so this thermometer has a higher cost-effectiveness. It has been used in power equipment to monitor the temperature of copper plates in high-voltage cabinets with good results.
Innovative idea: Applying thermopile infrared
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