Temperature measurement method, device and equipment in high-pressure environment, storage medium and product

By modulating and analyzing the original monochromatic optical signal, the problems of low accuracy and low efficiency of temperature measurement in high-voltage charge environments are solved, and high accuracy and high efficiency temperature measurement are achieved.

CN119533700APending Publication Date: 2025-02-28新疆准能投资有限公司
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Patent Information

Application Number
CN202411834137.7
Authority / Receiving Office
CN · China
Patent Type
Applications(China)
Current Assignee / Owner
Filing Date
2024-12-13
Publication Date
2025-02-28

AI Technical Summary

Technical Problem

In high-voltage charge environments, traditional temperature measurement technology is difficult to accurately measure temperature and is relatively inefficient.

Method used

By modulating the original monochromatic optical signal, at least two modulated optical signals are generated, the thermal absorption signals of these optical signals are obtained through the area to be detected, and the thermal absorption signals and modulated optical signals are analyzed using the preset temperature change analysis model to determine the current temperature parameters of the area to be detected.

Benefits of technology

The accuracy of temperature measurement in high-load environments is improved, the impact of high-charge environments on temperature measurement is reduced, and the problems of low accuracy and low efficiency in the prior art are avoided.

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Abstract

The invention relates to the technical field of smart power plants, in particular to a temperature measurement method, device and equipment in a high-voltage environment, a storage medium and a product. A temperature change value after an optical signal passes through a to-be-detected area is obtained by analyzing a modulated optical signal and a heat absorption signal passing through the to-be-detected area; the influence of a high-charge environment on temperature measurement is reduced, and then the current temperature parameter of the region is determined by combining the temperature change value of the optical signal and the historical temperature parameter of the region, so that the accuracy of temperature measurement in the high-load environment is improved. The technical problems of low accuracy and low efficiency of temperature measurement in a high-voltage charge environment in the prior art are solved.
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Description

Technical Field

[0001] The present invention relates to the field of smart power plant technology, and in particular to temperature measurement methods, devices, equipment, storage media and products under high-voltage environments. Background Art

[0002] In order to ensure the normal operation of the power plant, it is necessary to monitor the temperature of the areas where the equipment is located in the power plant in real time to avoid damage to equipment components due to excessive temperature. Excessive temperature may even cause the energy storage equipment to burn. However, due to the large amount of free charges in the power plant and the formation of a high electromagnetic environment, traditional temperature measurement technology will be affected and it is difficult to accurately measure the ambient temperature of each area. If manual inspection is used, the workload is large and monitoring cannot be implemented.

[0003] The above contents are only used to assist in understanding the technical solution of the present invention and do not constitute an admission that the above contents are prior art. Summary of the invention

[0004] The main purpose of the present invention is to provide a temperature measurement method, device, equipment, storage medium and product under a high-voltage environment, aiming to solve the technical problems in the prior art of low accuracy and low efficiency in temperature measurement under a high-voltage charge environment.

[0005] To achieve the above object, the present invention provides a temperature measurement method under high pressure environment, the method comprising the following steps:

[0006] Modulating the original monochromatic light signal to obtain at least two modulated light signals;

[0007] Acquire heat absorption signals of the two modulated light signals passing through the area to be detected;

[0008] The heat absorption signal and the modulated light signal are analyzed by a preset temperature change analysis model to obtain a temperature change value between the two light signals and the corresponding heat signal;

[0009] The current temperature parameter of the area to be detected is determined according to the temperature change value and the historical temperature parameter.

[0010] Optionally, the step of modulating the original monochromatic light signal to obtain at least two modulated light signals includes:

[0011] generating a first sinusoidal modulated current having a first angular frequency and a second sinusoidal modulated current corresponding to a second angular frequency, wherein the second angular frequency is greater than the first angular frequency;

[0012] The first sinusoidal modulation current and the second sinusoidal modulation current are respectively applied to a laser emitting device that emits the original monochromatic light signal to obtain a first modulated light signal and a second modulated light signal.

[0013] Optionally, the heat absorption signal includes a first heat absorption signal corresponding to the first modulated optical signal and a second heat absorption signal corresponding to the second adjusted optical signal;

[0014] The heat absorption signal and the modulated light signal are analyzed by a preset temperature change analysis model to obtain a temperature change value between the two light signals and the corresponding heat signal, including:

[0015] Acquire a second harmonic peak ratio between the first heat absorption signal and the second heat absorption signal;

[0016] determining a transition energy level difference between the first heat absorption signal and the second heat absorption signal;

[0017] Query the first absorption line intensity corresponding to the first thermal absorption signal and the second absorption line intensity corresponding to the second thermal absorption signal at the reference temperature;

[0018] The temperature change value between the two light signals and the corresponding thermal signals is calculated according to the second harmonic peak ratio, the transition energy level difference, the first absorption line intensity, the second absorption line intensity and a preset constant.

[0019] Optionally, acquiring a second harmonic peak ratio between the first heat absorption signal and the second heat absorption signal comprises:

[0020] Determine, by a spectrometer, a first absorption line intensity corresponding to the first thermal absorption signal and a second absorption line intensity corresponding to the second thermal absorption signal at a reference temperature;

[0021] A second harmonic peak ratio is generated according to the first absorption line intensity and the second absorption line intensity.

[0022] Optionally, the temperature change value is calculated as follows:

[0023]

[0024] Where T is the temperature change value, T0 is the reference temperature, S1(T0) is the first absorption line intensity at the reference temperature T0, S2(T0) is the second absorption line intensity at the reference temperature T0, E``2 is the low energy state energy of the transition, and E``1 is the high energy state energy before the transition. is the center frequency of the absorption line; h is Planck's constant, c is the speed of light, k is the Boltzmann constant, K is the ratio of the integral of the linear function of the first thermal absorption signal and the second thermal absorption signal, It is the ratio of the light intensity of the center frequency of the first thermal absorption signal and the second thermal absorption signal.

[0025] Optionally, determining the current temperature parameter of the area to be detected according to the temperature change value and the historical temperature parameter includes:

[0026] Extract the last measured temperature from the historical temperature parameters;

[0027] The current temperature parameter of the area to be detected is determined according to the sum of the last measured temperature and the temperature change value.

[0028] In addition, to achieve the above-mentioned purpose, the present invention further proposes a temperature measuring device under high pressure environment, the temperature measuring device under high pressure environment comprising:

[0029] A modulation module, used for modulating the original monochromatic light signal to obtain at least two modulated light signals;

[0030] An acquisition module, used for acquiring heat absorption signals of the two modulated light signals passing through the area to be detected;

[0031] An analysis module, used to analyze the heat absorption signal and the modulated light signal through a preset temperature change analysis model to obtain a temperature change value between the two light signals and the corresponding heat signal;

[0032] The temperature measurement module is used to determine the current temperature parameter of the area to be detected according to the temperature change value and the historical temperature parameter.

[0033] In addition, to achieve the above-mentioned purpose, the present invention also proposes a temperature measuring device under a high-pressure environment, wherein the temperature measuring device under a high-pressure environment comprises: a memory, a processor, and a temperature measurement program under a high-pressure environment stored in the memory and executable on the processor, wherein the temperature measurement program under a high-pressure environment is configured to implement the steps of the temperature measurement method under a high-pressure environment as described above.

[0034] In addition, to achieve the above-mentioned purpose, the present invention also proposes a storage medium, which stores a temperature measurement program under a high-pressure environment. When the temperature measurement program under a high-pressure environment is executed by a processor, the steps of the temperature measurement method under a high-pressure environment as described above are implemented.

[0035] In addition, to achieve the above-mentioned purpose, the present application also provides a computer program product, which includes a computer program, and when the computer program is executed by a processor, it implements the steps of the temperature measurement method under a high-pressure environment as described above.

[0036] One or more technical solutions proposed in the present invention have at least the following technical effects: the present invention obtains at least two modulated light signals by modulating the original monochromatic light signal; obtains the heat absorption signals of the two modulated light signals passing through the area to be detected; analyzes the heat absorption signal and the modulated light signal through a preset temperature change analysis model to obtain the temperature change value between the two light signals and the corresponding heat signals; determines the current temperature parameters of the area to be detected according to the temperature change value and the historical temperature parameters, and obtains the temperature change value of the light signal after passing through the area to be detected by analyzing the modulated light signal and the heat absorption signal passing through the area to be detected, thereby reducing the impact of the high charge environment on the temperature measurement, and finally determines the current temperature parameters of the area in combination with the temperature change value of the light signal and the historical temperature parameters of the area, thereby improving the accuracy of temperature measurement in a high load environment and avoiding the technical problems of low accuracy and low efficiency in temperature measurement in a high voltage charge environment in the prior art. BRIEF DESCRIPTION OF THE DRAWINGS

[0037] The accompanying drawings, which are incorporated in and constitute a part of this specification, illustrate embodiments consistent with the present application and, together with the description, serve to explain the principles of the present application.

[0038] In order to more clearly illustrate the embodiments of the present application or the technical solutions in the prior art, the drawings required for use in the embodiments or the description of the prior art will be briefly introduced below. Obviously, for ordinary technicians in this field, other drawings can be obtained based on these drawings without paying any creative labor.

[0039] Figure 1 It is a flow chart of a first embodiment of a temperature measurement method under a high pressure environment of the present invention;

[0040] Figure 2 It is a flow chart of a second embodiment of the temperature measurement method under high pressure environment of the present invention;

[0041] Figure 3 It is a structural block diagram of a first embodiment of a temperature measuring device under a high pressure environment of the present invention;

[0042] Figure 4 It is a structural schematic diagram of a temperature measuring device in a high-pressure environment of a hardware operating environment involved in an embodiment of the present invention.

[0043] The realization of the purpose, functional features and advantages of the present invention will be further explained in conjunction with embodiments and with reference to the accompanying drawings. DETAILED DESCRIPTION

[0044] It should be understood that the specific embodiments described herein are only used to explain the technical solutions of the present application and are not used to limit the present application.

[0045] Based on this, the embodiment of the present invention provides a temperature measurement method under high pressure environment, referring to Figure 1 , Figure 1 It is a flow chart of a first embodiment of a temperature measurement method under a high pressure environment of the present invention.

[0046] In this embodiment, the temperature measurement method under high pressure environment includes:

[0047] Step S10: modulate the original monochromatic light signal to obtain at least two modulated light signals.

[0048] It should be noted that the execution subject of this embodiment can be a computing service device with data processing, network communication and program running functions, such as a tablet computer, a personal computer, a mobile phone, etc., or an electronic device capable of realizing the above functions, a control computer, etc. The following takes the control computer as an example to illustrate this embodiment and the following embodiments.

[0049] It should be noted that traditional temperature measurement technology may cause inaccurate temperature measurement or data transmission interference due to high-voltage electric fields and electromagnetic interference. Some existing technologies can also achieve temperature measurement in high-voltage charge environments, such as optical fiber temperature measurement, infrared temperature measurement, etc. However, the cost of optical fiber temperature measurement technology is relatively high, and accurate temperature measurement can only be achieved after installation and testing by professionals. Infrared temperature measurement technology is affected by dust, humidity, temperature and other factors in the environment, and the accuracy of temperature measurement is relatively low.

[0050] Based on this, this embodiment analyzes the modulated light signal and the heat absorption signal passing through the area to be detected to obtain the temperature change value of the light signal after passing through the area to be detected, thereby reducing the impact of the high charge environment on the temperature measurement, and finally combining the temperature change value of the light signal and the historical temperature parameters of the area to determine the current temperature parameters of the area, thereby improving the accuracy of temperature measurement in a high-load environment and avoiding the technical problems of low accuracy and low efficiency in temperature measurement in a high-voltage charge environment in the prior art.

[0051] The original monochromatic light signal may be generated by a laser, or may be generated by other devices that can generate monochromatic light signals, and this embodiment does not impose any specific limitation on this.

[0052] Furthermore, the step of modulating the original monochromatic light signal to obtain at least two modulated light signals includes:

[0053] generating a first sinusoidal modulated current having a first angular frequency and a second sinusoidal modulated current corresponding to a second angular frequency, wherein the second angular frequency is greater than the first angular frequency;

[0054] The first sinusoidal modulation current and the second sinusoidal modulation current are respectively applied to a laser emitting device that emits the original monochromatic light signal to obtain a first modulated light signal and a second modulated light signal.

[0055] In a specific implementation, modulating the original monochromatic light signal refers to applying a sinusoidal modulation current of a first angular frequency to the laser, so that the frequency and intensity of the original monochromatic light signal are deflected to obtain a first modulated light signal, and applying a sinusoidal modulation current of a second angular frequency to the laser, so that the frequency and intensity of the original monochromatic light signal are deflected to obtain a second modulated light signal, wherein the second angular frequency is greater than the first angular frequency, specifically, the second angular frequency is twice the first angular frequency, thereby reducing the noise between the two modulated light signals and reducing the workload of subsequent signal processing.

[0056] Step S20: obtaining the thermal absorption signal of the two modulated light signals passing through the area to be detected.

[0057] In the field of optics, when a modulated light signal passes through a certain area, it will be affected by the temperature of the area and generate transition state energy, thereby changing some physical properties of the light signal. By detecting the spectral characteristics of the modulated light signal and the thermal absorption light signal, the influence of parameters such as the temperature and medium concentration of the area on the light signal can be effectively monitored, thereby measuring parameters such as the temperature and medium concentration of the area.

[0058] Step S30: Analyze the heat absorption signal and the modulated light signal using a preset temperature change analysis model to obtain a temperature change value between the two light signals and the corresponding heat signal.

[0059] The preset temperature change analysis model is used to detect the temperature change value between the thermal absorption signal and the modulated light signal. At the same time, the accuracy of temperature measurement based on the energy transition of a single light signal is not high. Especially when processing a single light signal, the baseline and the absorption line type will be fitted. If the fitting effect is not good, it will cause the signal-to-noise ratio to increase, thereby affecting the accuracy of temperature measurement.

[0060] Step S40: determining the current temperature parameter of the area to be detected according to the temperature change value and the historical temperature parameter.

[0061] Since the light signal will undergo energy transition when passing through the area to be detected, this transition energy will cause the light signal to undergo temperature change. Therefore, this embodiment measures the temperature change value between the two light signals and the corresponding thermal signals, and combines it with the historically measured temperature parameters to accurately determine the current temperature parameters of the area to be detected.

[0062] Further, determining the current temperature parameter of the area to be detected according to the temperature change value and the historical temperature parameter includes:

[0063] Extract the last measured temperature from the historical temperature parameters;

[0064] The current temperature parameter of the area to be detected is determined according to the sum of the last measured temperature and the temperature change value.

[0065] In a specific implementation, since the measured temperature data is stored in each temperature measurement cycle, after determining the temperature change of the light signal passing through the area to be detected, the current temperature parameters of the area to be detected can be accurately measured in combination with the last measured temperature.

[0066] This embodiment obtains at least two modulated light signals by modulating the original monochromatic light signal; obtains the heat absorption signal of the two modulated light signals passing through the area to be detected; analyzes the heat absorption signal and the modulated light signal through a preset temperature change analysis model to obtain the temperature change value between the two light signals and the corresponding heat signal; determines the current temperature parameter of the area to be detected according to the temperature change value and the historical temperature parameter, and obtains the temperature change value of the light signal after passing through the area to be detected by analyzing the modulated light signal and the heat absorption signal passing through the area to be detected, thereby reducing the impact of the high-charge environment on the temperature measurement, and finally determines the current temperature parameter of the area in combination with the temperature change value of the light signal and the historical temperature parameters of the area, thereby improving the accuracy of temperature measurement in a high-load environment and avoiding the technical problems of low accuracy and low efficiency in temperature measurement in a high-voltage charge environment in the prior art.

[0067] Based on the first embodiment of the present application, in the second embodiment of the present application, the same or similar contents as those in the above-mentioned embodiment 1 can be referred to the above introduction, and will not be repeated in the following. Figure 2 , step S30, comprising:

[0068] Step S301: obtaining a second harmonic peak ratio between the first heat absorption signal and the second heat absorption signal.

[0069] Step S302: determining a transition energy level difference between the first heat absorption signal and the second heat absorption signal.

[0070] Step S303: querying the first absorption line intensity corresponding to the first thermal absorption signal and the second absorption line intensity corresponding to the second thermal absorption signal at the reference temperature.

[0071] Step S304: Calculate the temperature change value between the two light signals and the corresponding thermal signals according to the second harmonic peak ratio, the transition energy level difference, the first absorption line intensity, the second absorption line intensity and a preset constant.

[0072] It should be noted that the second harmonic peak ratio refers to the absorption signals of two absorption lines obtained after two laser beams pass through the measurement area at the same time along the same path. The peak values ​​of the absorption signals of the two absorption lines are compared, and the ratio of the peak values ​​of the two absorption line spectra is taken as the second harmonic peak ratio. In order to accurately obtain the intensities of the two absorption line spectra, this embodiment needs to calculate the second-order coefficient of the Fourier series of the transmitted light intensity of the thermal absorption light signal, and then compare the peak values ​​of the two absorption line spectra.

[0073] Further, the obtaining of the second harmonic peak ratio between the first heat absorption signal and the second heat absorption signal comprises:

[0074] Determine, by a spectrometer, a first absorption line intensity corresponding to the first thermal absorption signal and a second absorption line intensity corresponding to the second thermal absorption signal at a reference temperature;

[0075] A second harmonic peak ratio is generated according to the first absorption line intensity and the second absorption line intensity.

[0076] In a specific implementation, the calculation formula for the second harmonic peak ratio is:

[0077]

[0078] Where R is the second harmonic peak ratio, is the ratio of the light intensity of the center frequency of the second heat absorption signal to that of the first heat absorption signal, a is the modulation amplitude of the modulated light signal compared to the frequency of the original monochromatic light signal, is the second-order coefficient of the Fourier series of the transmitted light intensity corresponding to the second thermal absorption signal, is the second-order coefficient of the Fourier series of the transmitted light intensity corresponding to the first thermal absorption signal.

[0079] Furthermore, the calculation formula of the temperature change value is:

[0080]

[0081] Where T is the temperature change value, T0 is the reference temperature, S1(T0) is the first absorption line intensity at the reference temperature T0, S2(T0) is the second absorption line intensity at the reference temperature T0, E``2 is the low energy state energy of the transition, and E``1 is the high energy state energy before the transition. is the center frequency of the absorption line; h is Planck's constant, c is the speed of light, k is the Boltzmann constant, K is the ratio of the integral of the linear function of the first thermal absorption signal and the second thermal absorption signal, It is the ratio of the light intensity of the center frequency of the first thermal absorption signal and the second thermal absorption signal.

[0082] This embodiment obtains the second harmonic peak ratio between the first heat absorption signal and the second heat absorption signal; determines the transition energy level difference between the first heat absorption signal and the second heat absorption signal; queries the first absorption line intensity corresponding to the first heat absorption signal and the second absorption line intensity corresponding to the second heat absorption signal at the reference temperature; calculates the temperature change value between the two light signals and the corresponding heat signals according to the second harmonic peak ratio, the transition energy level difference, the first absorption line intensity, the second absorption line intensity and the preset constant, and calculates the temperature change value of the heat absorption signal after the modulated light signal passes through the detection area through the pre-constructed temperature change analytical model, thereby reducing the impact of the high-voltage charge environment on the temperature measurement and improving the temperature measurement effect. .

[0083] This application also provides a temperature measurement device under high pressure environment, please refer to Figure 3 , the temperature measuring device under high pressure environment comprises:

[0084] The modulation module 10 is used to modulate the original monochromatic light signal to obtain at least two modulated light signals.

[0085] The acquisition module 20 is used to acquire the thermal absorption signal of the two modulated light signals passing through the area to be detected.

[0086] The analysis module 30 is used to analyze the heat absorption signal and the modulated light signal through a preset temperature change analysis model to obtain a temperature change value between the two light signals and the corresponding heat signal.

[0087] The temperature measurement module 40 is used to determine the current temperature parameter of the area to be detected according to the temperature change value and the historical temperature parameter.

[0088] This embodiment obtains at least two modulated light signals by modulating the original monochromatic light signal; obtains the heat absorption signal of the two modulated light signals passing through the area to be detected; analyzes the heat absorption signal and the modulated light signal through a preset temperature change analysis model to obtain the temperature change value between the two light signals and the corresponding heat signal; determines the current temperature parameter of the area to be detected according to the temperature change value and the historical temperature parameter, and obtains the temperature change value of the light signal after passing through the area to be detected by analyzing the modulated light signal and the heat absorption signal passing through the area to be detected, thereby reducing the impact of the high-charge environment on the temperature measurement, and finally determines the current temperature parameter of the area in combination with the temperature change value of the light signal and the historical temperature parameters of the area, thereby improving the accuracy of temperature measurement in a high-load environment and avoiding the technical problems of low accuracy and low efficiency in temperature measurement in a high-voltage charge environment in the prior art.

[0089] In one embodiment, the modulation module 10 is also used to generate a first sinusoidal modulation current of a first angular frequency and a second sinusoidal modulation current corresponding to a second angular frequency, wherein the second angular frequency is greater than the first angular frequency; the first sinusoidal modulation current and the second sinusoidal modulation current are respectively applied to a laser emitting device that emits the original monochromatic light signal to obtain a first modulated light signal and a second modulated light signal.

[0090] In one embodiment, the analysis module 30 is further used to obtain the second harmonic peak ratio between the first thermal absorption signal and the second thermal absorption signal; determine the transition energy level difference between the first thermal absorption signal and the second thermal absorption signal; query the first absorption line intensity corresponding to the first thermal absorption signal and the second absorption line intensity corresponding to the second thermal absorption signal at a reference temperature; calculate the temperature change value between the two light signals and the corresponding thermal signals according to the second harmonic peak ratio, the transition energy level difference, the first absorption line intensity, the second absorption line intensity and a preset constant.

[0091] In one embodiment, the analysis module 30 is further used to determine the first absorption line intensity corresponding to the first thermal absorption signal and the second absorption line intensity corresponding to the second thermal absorption signal at a reference temperature through a spectrometer; and generate a second harmonic peak ratio according to the first absorption line intensity and the second absorption line intensity.

[0092] In one embodiment, the analysis module 30 is further used for calculating the temperature change value using the following formula:

[0093]

[0094] Where T is the temperature change value, T0 is the reference temperature, S1(T0) is the first absorption line intensity at the reference temperature T0, S2(T0) is the second absorption line intensity at the reference temperature T0, E``2 is the low energy state energy of the transition, and E``1 is the high energy state energy before the transition. is the center frequency of the absorption line; h is Planck's constant, c is the speed of light, k is the Boltzmann constant, K is the ratio of the integral of the linear function of the first thermal absorption signal and the second thermal absorption signal, It is the ratio of the light intensity of the center frequency of the first thermal absorption signal and the second thermal absorption signal.

[0095] In one embodiment, the temperature measurement module 40 is further used to extract the last measured temperature in the historical temperature parameters; and determine the current temperature parameter of the area to be detected according to the sum of the last measured temperature and the temperature change value.

[0096] The present application provides a temperature measuring device under a high-pressure environment, and the temperature measuring device under a high-pressure environment includes: at least one processor; and a memory connected to the at least one processor in communication; wherein the memory stores instructions that can be executed by the at least one processor, and the instructions are executed by the at least one processor so that the at least one processor can execute the temperature measurement method under the high-pressure environment in the above-mentioned embodiment one.

[0097] Reference below Figure 4 , which shows a schematic diagram of the structure of a temperature measuring device under a high pressure environment suitable for implementing the embodiment of the present application. The temperature measuring device under a high pressure environment in the embodiment of the present application may include but is not limited to mobile terminals such as mobile phones, laptop computers, digital broadcast receivers, PDAs (Personal Digital Assistants), PADs (Portable Application Descriptions), PMPs (Portable Media Players), vehicle-mounted terminals (such as vehicle-mounted navigation terminals), etc., and fixed terminals such as digital TVs, desktop computers, etc. Figure 4 The temperature measuring device under high pressure environment shown is only an example and should not bring any limitation to the function and scope of use of the embodiments of the present application.

[0098] like Figure 4As shown, the temperature measuring device under high pressure environment may include a processing device 1001 (such as a central processing unit, a graphics processing unit, etc.), which can perform various appropriate actions and processes according to the program stored in the read-only memory (ROM: Read Only Memory) 1002 or the program loaded from the storage device 1003 to the random access memory (RAM: Random Access Memory) 1004. In RAM1004, various programs and data required for the operation of the temperature measuring device under high pressure environment are also stored. The processing device 1001, ROM1002 and RAM1004 are connected to each other through a bus 1005. An input / output (I / O) interface 1006 is also connected to the bus. Typically, the following systems can be connected to the I / O interface 1006: input devices 1007 including, for example, a touch screen, a touchpad, a keyboard, a mouse, an image sensor, a microphone, an accelerometer, a gyroscope, etc.; output devices 1008 including, for example, a liquid crystal display (LCD), a speaker, a vibrator, etc.; storage devices 1003 including, for example, a magnetic tape, a hard disk, etc.; and communication devices 1009. The communication device 1009 can allow the temperature measuring device in a high-pressure environment to communicate with other devices wirelessly or by wire to exchange data. Although the figure shows a temperature measuring device in a high-pressure environment with various systems, it should be understood that it is not required to implement or have all the systems shown. More or fewer systems may be implemented or have alternatively.

[0099] In particular, according to the embodiments disclosed in the present application, the process described above with reference to the flowchart can be implemented as a computer software program. For example, the embodiments disclosed in the present application include a computer program product, which includes a computer program carried on a computer-readable medium, and the computer program includes a program code for executing the method shown in the flowchart. In such an embodiment, the computer program can be downloaded and installed from a network through a communication device, or installed from a storage device 1003, or installed from a ROM 1002. When the computer program is executed by the processing device 1001, the above-mentioned functions defined in the method of the embodiment disclosed in the present application are executed.

[0100] The temperature measuring device under high pressure environment provided by the present application adopts the temperature measuring method under high pressure environment in the above embodiment, which can solve the technical problem of temperature measurement under high pressure environment. Compared with the prior art, the beneficial effect of the temperature measuring device under high pressure environment provided by the present application is the same as the beneficial effect of the temperature measuring method under high pressure environment provided by the above embodiment, and other technical features of the temperature measuring device under high pressure environment are the same as the features disclosed in the method of the previous embodiment, which will not be described in detail here.

[0101] It should be understood that the various parts disclosed in this application can be implemented by hardware, software, firmware or a combination thereof. In the description of the above embodiments, specific features, structures, materials or characteristics can be combined in any one or more embodiments or examples in a suitable manner.

[0102] The above is only a specific implementation of the present application, but the protection scope of the present application is not limited thereto. Any person skilled in the art who is familiar with the present technical field can easily think of changes or substitutions within the technical scope disclosed in the present application, which should be included in the protection scope of the present application. Therefore, the protection scope of the present application should be based on the protection scope of the claims.

[0103] The present application provides a computer-readable storage medium having computer-readable program instructions (ie, computer programs) stored thereon, and the computer-readable program instructions are used to execute the temperature measurement method under a high-pressure environment in the above-mentioned embodiment.

[0104] The computer-readable storage medium provided in the present application may be, for example, a USB flash drive, but is not limited to electrical, magnetic, optical, electromagnetic, infrared, or semiconductor systems, systems or devices, or any combination of the above. More specific examples of computer-readable storage media may include, but are not limited to: an electrical connection with one or more wires, a portable computer disk, a hard disk, a random access memory (RAM), a read-only memory (ROM), an erasable programmable read-only memory (EPROM or flash memory), an optical fiber, a portable compact disk read-only memory (CD-ROM), an optical storage device, a magnetic storage device, or any suitable combination of the above. In this embodiment, the computer-readable storage medium may be any tangible medium containing or storing a program that can be used by or in combination with an instruction execution system, system or device. The program code contained on the computer-readable storage medium may be transmitted using any appropriate medium, including but not limited to: wires, optical cables, RF (Radio Frequency), etc., or any suitable combination of the above.

[0105] The computer-readable storage medium may be included in the temperature measuring device under high pressure environment; or may exist independently without being assembled into the temperature measuring device under high pressure environment.

[0106] The computer-readable storage medium carries one or more programs. When the one or more programs are executed by the temperature measuring device under a high-pressure environment, the temperature measuring device under a high-pressure environment can measure temperature under a high-pressure environment.

[0107] Computer program code for performing the operations of the present application may be written in one or more programming languages ​​or a combination thereof, including object-oriented programming languages ​​such as Java, Smalltalk, C++, and conventional procedural programming languages ​​such as "C" or similar programming languages. The program code may be executed entirely on the user's computer, partially on the user's computer, as a separate software package, partially on the user's computer and partially on a remote computer, or entirely on a remote computer or server. In the case of a remote computer, the remote computer may be connected to the user's computer through any type of network, including a local area network (LAN) or a wide area network (WAN), or may be connected to an external computer (e.g., via the Internet using an Internet service provider).

[0108] The flow chart and block diagram in the accompanying drawings illustrate the possible architecture, function and operation of the system, method and computer program product according to various embodiments of the present application. In this regard, each box in the flow chart or block diagram can represent a module, a program segment or a part of a code, and the module, the program segment or a part of the code contains one or more executable instructions for realizing the specified logical function. It should also be noted that in some alternative implementations, the functions marked in the box can also occur in a sequence different from that marked in the accompanying drawings. For example, two boxes represented in succession can actually be executed substantially in parallel, and they can sometimes be executed in the opposite order, depending on the functions involved. It should also be noted that each box in the block diagram and / or flow chart, and the combination of the boxes in the block diagram and / or flow chart can be implemented with a dedicated hardware-based system that performs a specified function or operation, or can be implemented with a combination of dedicated hardware and computer instructions.

[0109] The modules involved in the embodiments described in this application may be implemented by software or hardware, wherein the name of the module does not constitute a limitation on the unit itself in some cases.

[0110] The readable storage medium provided in the present application is a computer-readable storage medium, which stores computer-readable program instructions (i.e., computer programs) for executing the temperature measurement method under the above-mentioned high-pressure environment, and can solve the technical problem of temperature measurement under the high-pressure environment. Compared with the prior art, the beneficial effects of the computer-readable storage medium provided in the present application are the same as the beneficial effects of the temperature measurement method under the high-pressure environment provided in the above-mentioned embodiment, and will not be repeated here.

[0111] The present application also provides a computer program product, including a computer program, which implements the steps of the temperature measurement method under a high-pressure environment as described above when executed by a processor.

[0112] The computer program product provided by the present application can solve the technical problem of temperature measurement under high pressure environment. Compared with the prior art, the beneficial effects of the computer program product provided by the present application are the same as the beneficial effects of the temperature measurement method under high pressure environment provided by the above embodiment, which will not be repeated here.

[0113] The above descriptions are only some embodiments of the present application, and are not intended to limit the patent scope of the present application. All equivalent structural changes made using the contents of the present application specification and drawings under the technical concept of the present application, or direct / indirect applications in other related technical fields are included in the patent protection scope of the present application.

Claims

1. A temperature measurement method under high pressure environment, characterized in that: The temperature measurement method under high pressure environment comprises: Modulating the original monochromatic light signal to obtain at least two modulated light signals; Acquire heat absorption signals of the two modulated light signals passing through the area to be detected; The heat absorption signal and the modulated light signal are analyzed by a preset temperature change analysis model to obtain a temperature change value between the two light signals and the corresponding heat signal; The current temperature parameter of the area to be detected is determined according to the temperature change value and the historical temperature parameter.

2. The method according to claim 1, characterized in that The method of modulating the original monochromatic light signal to obtain at least two modulated light signals comprises: generating a first sinusoidal modulated current having a first angular frequency and a second sinusoidal modulated current corresponding to a second angular frequency, wherein the second angular frequency is greater than the first angular frequency; The first sinusoidal modulation current and the second sinusoidal modulation current are respectively applied to a laser emitting device that emits the original monochromatic light signal to obtain a first modulated light signal and a second modulated light signal.

3. The method according to claim 1, characterized in that The heat absorption signal includes a first heat absorption signal corresponding to the first modulated light signal and a second heat absorption signal corresponding to the second adjusted light signal; The heat absorption signal and the modulated light signal are analyzed by a preset temperature change analysis model to obtain a temperature change value between the two light signals and the corresponding heat signal, including: Acquire a second harmonic peak ratio between the first heat absorption signal and the second heat absorption signal; determining a transition energy level difference between the first heat absorption signal and the second heat absorption signal; Query the first absorption line intensity corresponding to the first thermal absorption signal and the second absorption line intensity corresponding to the second thermal absorption signal at the reference temperature; The temperature change value between the two light signals and the corresponding thermal signals is calculated according to the second harmonic peak ratio, the transition energy level difference, the first absorption line intensity, the second absorption line intensity and a preset constant.

4. The method according to claim 3, characterized in that The obtaining of the second harmonic peak ratio between the first heat absorption signal and the second heat absorption signal comprises: Determine, by a spectrometer, a first absorption line intensity corresponding to the first thermal absorption signal and a second absorption line intensity corresponding to the second thermal absorption signal at a reference temperature; A second harmonic peak ratio is generated according to the first absorption line intensity and the second absorption line intensity.

5. The method according to claim 3, characterized in that The calculation formula of the temperature change value is: Where T is the temperature change value, T0 is the reference temperature, S1(T0) is the first absorption line intensity at the reference temperature T0, S2(T0) is the second absorption line intensity at the reference temperature T0, E``2 is the low energy state energy of the transition, and E``1 is the high energy state energy before the transition. is the center frequency of the absorption line; h is Planck's constant, c is the speed of light, k is the Boltzmann constant, K is the ratio of the integral of the linear function of the first thermal absorption signal and the second thermal absorption signal, It is the ratio of the light intensity of the center frequency of the first thermal absorption signal and the second thermal absorption signal.

6. The method according to any one of claims 1 to 5, characterized in that The determining the current temperature parameter of the area to be detected according to the temperature change value and the historical temperature parameter includes: Extract the last measured temperature from the historical temperature parameters; The current temperature parameter of the area to be detected is determined according to the sum of the last measured temperature and the temperature change value.

7. A temperature measuring device under high pressure environment, characterized in that: The temperature measuring device under the high pressure environment comprises: A modulation module, used for modulating the original monochromatic light signal to obtain at least two modulated light signals; An acquisition module, used for acquiring heat absorption signals of the two modulated light signals passing through the area to be detected; An analysis module, used to analyze the heat absorption signal and the modulated light signal through a preset temperature change analysis model to obtain a temperature change value between the two light signals and the corresponding heat signal; The temperature measurement module is used to determine the current temperature parameter of the area to be detected according to the temperature change value and the historical temperature parameter.

8. A temperature measuring device under high pressure environment, characterized in that: The temperature measurement device under high pressure environment comprises: a memory, a processor and a temperature measurement program under high pressure environment stored in the memory and executable on the processor, wherein the temperature measurement program under high pressure environment is configured to implement the steps of the temperature measurement method under high pressure environment as described in any one of claims 1 to 6.

9. A storage medium, characterized in that: The storage medium stores a temperature measurement program under a high-pressure environment, and when the temperature measurement program under a high-pressure environment is executed by a processor, the steps of the temperature measurement method under a high-pressure environment as described in any one of claims 1 to 6 are implemented.

10. A computer program product, characterized in that The computer program product comprises a computer program, and when the computer program is executed by a processor, the steps of the temperature measurement method under a high pressure environment according to any one of claims 1 to 6 are implemented.

Citation Information

Patent Citations

  • Real-time temperature monitoring instrument for tunable semiconductor laser absorption spectrum

    CN102183316A

  • Combustion gas temperature and multi-component concentration measurement method and system based on TDLAS

    CN109270008A

  • Device for reconstructing combustion flame temperature field through laser absorption spectrum scanning light path

    CN112611477A

  • High-enthalpy plasma gas temperature measuring method, system and device based on absorption spectrum

    CN120800582A

  • Hot gas temperature measurement in gas turbine using tunable diode laser

    US20120060510A1