CN110686795A - Temperature measurement method of sapphire optical fiber in liquid metal based on ultrasonic principle - Google Patents
Temperature measurement method of sapphire optical fiber in liquid metal based on ultrasonic principle Download PDFInfo
- Publication number
- CN110686795A CN110686795A CN201910976150.9A CN201910976150A CN110686795A CN 110686795 A CN110686795 A CN 110686795A CN 201910976150 A CN201910976150 A CN 201910976150A CN 110686795 A CN110686795 A CN 110686795A
- Authority
- CN
- China
- Prior art keywords
- temperature
- optical fiber
- sapphire optical
- ultrasonic
- sapphire
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01K—MEASURING TEMPERATURE; MEASURING QUANTITY OF HEAT; THERMALLY-SENSITIVE ELEMENTS NOT OTHERWISE PROVIDED FOR
- G01K11/00—Measuring temperature based upon physical or chemical changes not covered by groups G01K3/00, G01K5/00, G01K7/00 or G01K9/00
- G01K11/32—Measuring temperature based upon physical or chemical changes not covered by groups G01K3/00, G01K5/00, G01K7/00 or G01K9/00 using changes in transmittance, scattering or luminescence in optical fibres
Abstract
The invention discloses a temperature measuring method of sapphire optical fiber in liquid metal based on ultrasonic principle, which adopts a sapphire optical fiber temperature measuring device based on ultrasonic principle, the sapphire optical fiber temperature measuring device based on ultrasonic principle comprises a sapphire optical fiber ultrasonic sensor, an ultrasonic pulse detector and a computer data acquisition system, the sapphire optical fiber ultrasonic sensor is connected with the excitation end of the ultrasonic pulse detector, the sapphire optical fiber ultrasonic sensor comprises a sapphire optical fiber transmission rod, at least one radial groove is arranged on the sensitive area of the sapphire optical fiber transmission rod at intervals, the sensitive area of the sapphire optical fiber transmission rod is used for temperature measurement, the data end of the ultrasonic pulse detector is connected with the computer data acquisition system, the sapphire optical fiber temperature measuring device is firstly subjected to laboratory static calibration to obtain the sound velocity values of the sapphire optical fiber transmission rod with different temperatures from normal temperature to high temperature, and then carrying out real-time measurement on the high-temperature molten liquid metal in practical occasions.
Description
Technical Field
The invention relates to the field of liquid high-temperature measurement, in particular to a method for measuring the temperature of a sapphire optical fiber in liquid metal based on an ultrasonic principle.
Background
With the continuous innovation of the technology in the manufacturing industry, many liquid high-temperature environments need to be subjected to temperature accurate testing. For example, the temperature test of molten aluminum, molten iron and molten steel in the metallurgical industry, the plasma temperature measurement in the electromagnetic field environment and the like, especially the aluminum alloy smelting technology has more and more prominent position in the manufacturing industry, and the quality of aluminum castings is directly influenced by the temperature of the molten aluminum. Therefore, temperature monitoring at different locations of the smelting process over a long period of time is required. Because the aluminum liquid has high-temperature corrosivity, the aluminum liquid can react with most metals. At present, the commonly used method for measuring the temperature of molten aluminum is provided with a k-shaped armored thermocouple and a portable handheld infrared thermometer.
(1) Intermittent temperature measurement is carried out by a k-type armored thermocouple: the thermal electrode and the insulating material are placed in a protected metal tube to be pressed. During measurement, the front end is immersed in the aluminum liquid for temperature measurement reading. Although the method is relatively simple, the protected metal pipe is easily damaged due to the characteristics of strong corrosion of high-temperature aluminum liquid, easy slag accumulation and the like, so that the measurement result is inaccurate, secondary pollution of the aluminum liquid can be caused, and the quality of the produced product cannot be ensured.
(2) Handheld portable infrared aluminium liquid thermoscope: the system comprises an amplifying system, a display system, a circuit system, an optical system and the like. The temperature of an object is determined primarily by receiving infrared radiation energy emitted outwardly from the object and converting it into a corresponding electrical signal. The method adopts non-contact measurement and is simple, but the measurement error is large, and the temperature value of the internal aluminum liquid cannot be accurately obtained.
The armored thermocouple can only carry out transient internal temperature point type measurement, and a plurality of test points need to be distributed for temperature distribution. The handheld infrared thermometer mainly collects the heat radiation energy on the surface of the aluminum liquid by using an infrared temperature measurement technology, cannot test the internal temperature, and has larger errors in the measurement results of the two. Meanwhile, the temperature of the aluminum liquid is monitored in real time, and the high-temperature strong corrosivity of the aluminum liquid must be considered. Because the aluminum liquid can react with almost all metals and oxides thereof.
Therefore, there is an urgent need to design a novel temperature sensor with high measurement accuracy and without causing secondary pollution to the aluminum liquid, and the temperature distribution gradient inside the aluminum liquid can be accurately measured, so as to obtain an aluminum alloy material with higher quality and performance through casting.
Disclosure of Invention
The invention aims to provide a method for measuring the temperature of a sapphire optical fiber in liquid metal based on an ultrasonic principle, which has high measurement precision and does not cause secondary pollution to the liquid metal.
In order to achieve the purpose, the technical scheme of the invention is as follows:
a temperature measuring method of sapphire optical fiber in liquid metal based on ultrasonic principle comprises a sapphire optical fiber ultrasonic sensor, an ultrasonic pulse detector and a computer data acquisition system, wherein the sapphire optical fiber ultrasonic sensor based on ultrasonic principle is connected with an excitation end of the ultrasonic pulse detector, the sapphire optical fiber ultrasonic sensor comprises a sapphire optical fiber transmission rod, at least one radial groove is arranged on a sensitive area of the sapphire optical fiber transmission rod at intervals, the sensitive area of the sapphire optical fiber transmission rod is used for temperature measurement, a data end of the ultrasonic pulse detector is connected with the computer data acquisition system, the sapphire optical fiber temperature measuring device is subjected to laboratory static calibration to obtain sound velocity values of the sapphire optical fiber transmission rod with different temperatures from normal temperature to high temperature, and then carrying out real-time measurement on the high-temperature molten liquid metal in practical occasions.
Furthermore, the electric signal of the ultrasonic pulse detector is converted into an ultrasonic signal through the transducer, the ultrasonic signal is transmitted into the sapphire optical fiber transmission rod from the excitation end to be transmitted, the ultrasonic signal is reflected back to the excitation end at the groove and the end face, and then the ultrasonic signal is converted into an electric signal which is transmitted into a computer data acquisition system through the data end to be analyzed by subsequent signals.
Further, the signal analysis is that the computer data acquisition system calculates the sound velocity value by calculating the delay data between the echo signal generated at the radial groove and the end surface reflection signal of the sapphire optical fiber transmission rod at different temperatures, and calculates to obtain delay data graphs at different temperature values, thereby obtaining the change curve of the velocity along with the temperature.
Furthermore, the number of the radial grooves is two, and a plurality of distributed temperature measuring points are formed.
Further, the distance between the radial groove position of the temperature measurement sensitive area and the end face of the sapphire optical fiber propagation rod is called as a reflection interval, and when the length of the reflection interval is selected, the following relational expression is satisfied:
in the formula: Δ L — reflection spacing; t is t1-ultrasonic pulse excitation time; v (T) -the ultrasonic wave velocity; Δ t — time difference.
Further, the obtaining of the sound velocity values of the sapphire optical fiber propagation rod at different temperatures from the normal temperature to the high temperature is to obtain a relationship curve of the temperature and the delay data by obtaining a time delay data graph from the normal temperature to 1600 ℃ and calculating. And during actual application, calculating the speed according to the obtained delay data according to v ═ 2l/t, and searching a relation curve of the temperature and the sound velocity to further obtain the actual temperature.
The temperature value is calculated by measuring the delay data of ultrasonic waves in the sensitive material by using an ultrasonic pulse temperature measurement technology to obtain the sound velocity, namely, the signal waveforms reflected from the grooves and the end faces are selected, the sound velocity value at the temperature can be obtained by calculating the delay data among the waveforms, and delay data graphs at different temperature values are obtained, so that the change curve of the ultrasonic propagation velocity along with the temperature is obtained.
Drawings
FIG. 1 is a graph of incident waves versus reflected and transmitted waves in accordance with the present invention;
FIG. 2 is a schematic view of a sapphire fiber waveguide of the present invention;
FIG. 3 is a schematic view of acoustic wave propagation of a sapphire optical fiber multi-distribution ultrasonic sensor of the present invention;
FIG. 4 is a sapphire optical fiber temperature measuring device based on the ultrasonic principle of the present invention;
FIG. 5 is a static calibration temperature measurement system of a molten aluminum laboratory of the sapphire optical fiber temperature measurement device based on the ultrasonic principle;
FIG. 6 is a waveform diagram of time-delay data from normal temperature to 1600 ℃ of the sapphire optical fiber temperature measuring device based on the ultrasonic principle;
FIG. 7 is a graph showing the relationship between the delay data and the temperature of the first groove and the second groove of the sapphire optical fiber propagation rod of the present invention;
FIG. 8 is a graph showing the relationship between the temperature and the sound velocity of the first and second grooves of the sapphire optical fiber propagation rod of the present invention;
FIG. 9 is a time-dependent temperature profile measured during a process in which the sapphire optical fiber temperature sensor of the present invention is inserted into molten aluminum.
Detailed Description
The invention is further described with reference to the following drawings and specific embodiments.
The ultrasonic temperature measurement technology obtains temperature information by testing the propagation speed of ultrasonic in liquid, and the ultrasonic sensor material has good thermal conductivity and sound transmission property and can quickly reach thermal balance with temperature measurement liquid. The material is called temperature-sensing material, and usually some metal wires, metal rods, single crystal material, etc. are selected. According to the scheme, a sapphire optical fiber which is drawn by an alumina single crystal is selected as a sensitive material by combining the high-temperature corrosion characteristic of molten aluminum.
As shown in fig. 4, the invention designs a sapphire optical fiber temperature measuring device based on the ultrasonic principle according to the ultrasonic temperature measuring principle, which comprises a sapphire optical fiber ultrasonic sensor 1, an ultrasonic pulse detector 2 and a computer data acquisition system 3, wherein the sapphire optical fiber ultrasonic sensor 1 is connected with an excitation end 21 of the ultrasonic pulse detector 2, the sapphire optical fiber ultrasonic sensor 1 comprises a sapphire optical fiber propagation rod 11, at least one radial groove 12 is arranged on a sensitive area of the sapphire optical fiber propagation rod 11 at intervals, the sensitive area of the sapphire optical fiber propagation rod 11 is used for temperature measurement, and a data end 22 of the ultrasonic pulse detector 2 is connected with the computer data acquisition system 3.
The working principle of the scheme is that as shown in fig. 1 and 4, an electric signal of the ultrasonic pulse detector 2 is converted into an acoustic signal through a transducer (not shown), the acoustic signal is transmitted into the sapphire optical fiber transmission rod 11 from the excitation end 21 to be transmitted, and is reflected back to the excitation end 21 at the groove 12 and the end face 13, and then the acoustic signal is converted into an electric signal which is transmitted into the computer data acquisition system 3 through the data end 22 to be analyzed by subsequent signals; the signal analysis is that the computer data acquisition system 3 calculates the sound velocity value by calculating the delay data between the echo signal generated at the radial groove 12 and the reflected signal of the end surface 13 of the sapphire optical fiber transmission rod 11 at different temperatures, and calculates the delay data graph at different temperature values, thereby obtaining the change curve of the velocity along with the temperature.
As shown in fig. 2, 3, and 4, the number of the radial grooves is two, which are the first groove 121 and the second groove 122, respectively, to form a multi-distributed temperature measurement point, an electrical signal of the ultrasonic pulse detector 2 is converted into an acoustic signal 41 by a transducer (not shown), the acoustic signal is transmitted from the excitation end 21 to the sapphire optical fiber propagation rod 11 for propagation, a second groove reflected wave 43 is generated at the second groove 122, a first groove reflected wave 42 is generated at the first groove 121, and an end surface reflected wave 44 is generated at the end surface 13, the first groove reflected wave 42, the second groove reflected wave 43, and the end surface reflected wave 44 are reflected back to the excitation end 21 by the sapphire optical fiber propagation rod 11, and the ultrasonic pulse detector 2 converts the acoustic signal into an electrical signal, and transmits the electrical signal to the computer data acquisition system 3 through the data end 22 for subsequent signal. The signal analysis is that the computer data acquisition system 3 calculates the sound velocity value by calculating the delay data between the echo signal groove two reflected wave 43 and the echo signal groove one reflected wave 42 generated by the groove two 122 and the groove one 121 and the echo signal end surface reflected wave 44 reflected by the end surface 13 of the sapphire optical fiber transmission rod 11 at different temperatures, and calculates the delay data graph at different temperature values, thereby obtaining the change curve of the speed of the multi-distribution temperature measurement points along with the temperature, and being more beneficial to the temperature measurement and analysis.
As shown in fig. 3, the distance between the radial groove position of the temperature-measuring sensitive region and the end face of the sapphire optical fiber propagation rod is called as a reflection interval, the distance between the groove two 122 and the groove one 121 is called as a reflection interval Δ L1, the distance between the groove one 121 and the end face 11 is called as a reflection interval Δ L2, and the size of the reflection interval has an important effect on ultrasonic temperature measurement: the reflection pitch is selected to be too large, and the delay data between the waveforms reflected by the second groove 122 and the first groove 121 and the end face 11 is too large. Although the analysis is facilitated, the length of the temperature measurement sensitive zone section is increased, and the temperature measured by the sapphire optical fiber ultrasonic sensor is the average temperature of the length of the sensitive zone section, so that the longer the temperature measurement zone section is, the lower the temperature measurement precision is, and the temperature gradient cannot be identified; on the other hand, when the reflection distance is too small, the waveforms and secondary echoes reflected by the second groove 122, the first groove 121 and the end face 11 are superposed together, so that accurate identification cannot be performed, and great trouble is brought to analysis data. Therefore, in conjunction with the above description, when selecting the reflection pitch length, the following relationship should be satisfied:
in the formula: Δ L — reflection spacing; t is t1-ultrasonic pulse excitation time; v (T) -the ultrasonic wave velocity; Δ t — time difference.
The sapphire optical fiber transmission rod is made of aluminum oxide (Al)2O3) The single crystal is formed by pulling, and has the characteristics of stable structure, high melting point (2053 ℃), good heat-conducting property and the like. Therefore, the temperature in the liquid metal is measured by adopting the sapphire optical fiber temperature measuring device based on the ultrasonic principle, the sapphire optical fiber temperature measuring device is firstly subjected to static calibration in a laboratory to obtain the sound velocity values of the sapphire optical fiber propagation rod with different temperatures from normal temperature to high temperature, and then high-temperature melting is carried out in practical occasionsAnd (4) measuring the liquid metal in real time.
For example, the temperature in liquid metal is measured by a sapphire optical fiber temperature measuring device based on the ultrasonic principle2O3) The manufactured sapphire optical fiber transmission rod does not react with molten aluminum, and a designed sapphire optical fiber temperature sensor needs to be subjected to a static calibration experiment before measuring the temperature of the molten aluminum, so that the waveform amplitude, the time delay data, the structural performance stability and the like of the sensor are checked.
As shown in figures 2, 3, 4 and 5, experimental calibration data from normal temperature to 1600 ℃ is obtained by laboratory calibration, a 1600 ℃ high-temperature resistance furnace 5 is used for data calibration, double rows of silicon-molybdenum rods are used for heating in the furnace, a 100 x 100mm temperature zone is formed by heat insulation of high-temperature refractory bricks at the periphery, and the temperature is set to be kept for 5 minutes at an integral temperature point in the heating time process, so that the internal temperature zone can be approximately regarded as a constant temperature field. The sapphire optical fiber propagation rod 11 of the sapphire optical fiber temperature sensor 1 and a standard platinum rhodium thermocouple are placed in a constant temperature field, and data are collected and recorded once when the temperature of the thermocouple changes by 100 ℃. When the distance between the second groove 122 and the first groove 121 of the sapphire optical fiber propagation rod 11 and the end face is fixed, the influence of the thermal expansion of the optical fiber temperature sensor itself can be almost ignored, the waveforms reflected by the second groove 122 and the first groove 121 at different temperatures are collected, and the delay data between the second groove 122 and the first groove 121, and between the first groove 121 and the end face 13 have a certain relation with the temperature value at the current state. By calibrating the delay data, a delay data graph (shown in fig. 6) of normal temperature to 1600 ℃ (high temperature) is obtained, a relation curve (shown in fig. 7) of temperature and delay data is obtained by calculation, and a relation curve (shown in fig. 8) of temperature and sound velocity can be obtained by calculation according to the delay data at different temperatures in fig. 7 and according to v being 2 l/t.
As shown in fig. 8, when the calibration is performed by using a high temperature resistance furnace, it is considered that the internal temperature field is uniform and constant, i.e. the temperature data of the first groove and the second groove obtained by the sapphire optical fiber temperature sensor in the temperature zone of 100 × 100 × 100mm are the same, and the curves of temperature and sound velocity should substantially coincide. Therefore, a relation graph of the temperature and the sound velocity obtained through a static calibration experiment is basically consistent with theoretical calculation data, and meanwhile, the feasibility of measuring the temperature of the sapphire optical fiber temperature sensor is verified.
And finally, measuring the temperature of the molten aluminum in real time by using a calibrated sapphire optical fiber temperature sensor, and analyzing the result.
In the actual temperature measurement process, a sapphire optical fiber propagation rod of a sapphire optical fiber temperature sensor needs to be inserted into molten aluminum for measurement, the lowest temperature of aluminum in a molten state is about 640 ℃, the highest upper limit temperature of an aluminum alloy resistance furnace adopted in the scheme can reach 740 ℃, and the temperature change process is not large. And carrying out temperature tests in two processes in the actual temperature measurement process. The first process is as follows: the sapphire optical fiber propagation rod is inserted into the aluminum liquid in the lowest melting state to reach thermal balance, and data are continuously collected to obtain a time response speed curve of the sapphire optical fiber temperature sensor; in addition, a plurality of single-point test temperature values under the state are also carried out; and a second process: the temperature value is set to the upper limit threshold value through the control cabinet, the heating process of the molten aluminum liquid is continuously collected, the temperature is raised in a furnace wall-air-dry pot heat exchange mode in the process, the heating process is slow, long-time continuous data collection is needed to obtain a temperature rise curve of the temperature along with the time, and multiple single-point temperature measurement is carried out on the aluminum liquid in the state of the highest temperature value.
After the aluminum liquid temperature is measured according to the first temperature measuring process, the data result is analyzed to obtain a temperature change curve along with time as shown in fig. 9, and the temperature change curve along with time as shown in fig. 9 can be obtained. In addition, it can be also found from the temperature rising curve of fig. 9 that the sapphire optical fiber temperature sensor reaches a thermal equilibrium state 43.8s after the molten metal aluminum liquid is inserted.
As the molten aluminum is subjected to heat transfer in a heat exchange mode, the data tested according to the test in FIG. 9 shows that the temperature gradient difference exists between the two sensitive sections of the first groove and the second groove in the longitudinal direction of the molten aluminum. The first groove is closer to the bottom of the dry pot, and the measured temperature value is higher after heat balance is carried out; the second groove is closer to the liquid level of the aluminum liquid, and the temperature is relatively lower, which indicates that the temperature distribution in the aluminum liquid is uneven in the heat exchange heating process.
After the first process is finished, the second process is carried out, and the temperature of the molten aluminum in the dry pot continuously rises along with the time by adjusting the rated temperature value of the control cabinet. After about 15min, the temperature reached 734 ℃ (740 ℃ peak upper control cabinet temperature, and continued increase would damage the control cabinet due to excessive power). And after the sapphire optical fiber transmission rod is measured in molten aluminum for a long time, the waveform amplitude is not changed, and no corrosion trace is found on the surface of the optical fiber in the temperature measurement sensitive area. Therefore, the sapphire optical fiber temperature sensor based on the ultrasonic temperature measurement principle can be used as a new method for measuring the temperature of molten aluminum.
The sapphire optical fiber temperature sensor that the present case designed according to supersound temperature measurement principle not only can use in aluminium liquid temperature measurement, moreover, because sapphire optical fiber itself has characteristics such as high melting point (2053 ℃), high temperature anti-oxidant, anti-electromagnetic interference, can be used for more occasions to carry out temperature test research. For example, the temperature test of molten iron and molten steel in the metallurgical industry, the plasma temperature measurement in the electromagnetic field environment and the like have wider research value and significance in the future.
The above are merely specific examples of the present invention, and do not limit the scope of the present invention. All equivalent changes made according to the design idea of the present application fall within the protection scope of the present application.
Claims (6)
1. A temperature measurement method of sapphire optical fiber in liquid metal based on ultrasonic principle is characterized in that: the sapphire optical fiber temperature measuring device based on the ultrasonic principle is adopted and comprises a sapphire optical fiber ultrasonic sensor, an ultrasonic pulse detector and a computer data acquisition system, wherein the sapphire optical fiber ultrasonic sensor is connected with an excitation end of the ultrasonic pulse detector, the sapphire optical fiber ultrasonic sensor comprises a sapphire optical fiber transmission rod, at least one radial groove is arranged on a sensitive area of the sapphire optical fiber transmission rod at intervals, the sensitive area of the sapphire optical fiber transmission rod is used for temperature measurement, a data end of the ultrasonic pulse detector is connected with the computer data acquisition system, the sapphire optical fiber temperature measuring device is subjected to laboratory static calibration firstly, sound velocity values of the sapphire optical fiber transmission rod at different temperatures from normal temperature to high temperature are obtained, and then high-temperature molten liquid metal real-time measurement is carried out on actual occasions.
2. The method for measuring the temperature of the sapphire optical fiber in the liquid metal based on the ultrasonic principle as claimed in claim 1, wherein: the electric signal of the ultrasonic pulse detector is converted into an ultrasonic signal through the transducer, the ultrasonic signal is transmitted into the sapphire optical fiber transmission rod from the excitation end to be transmitted, the ultrasonic signal is reflected back to the excitation end at the groove and the end face, and then the ultrasonic signal is converted into the electric signal which is transmitted into the computer data acquisition system through the data end to be analyzed by subsequent signals.
3. The method of claim 2 for measuring the temperature of sapphire fiber in liquid metal based on the ultrasonic principle, wherein the method comprises the following steps: the signal analysis is that the computer data acquisition system calculates the sound velocity value by calculating the delay data between the echo signal generated at the radial groove and the end surface reflection signal of the sapphire optical fiber transmission rod at different temperatures, and calculates to obtain the delay data graph at different temperature values, thereby obtaining the change curve of the velocity along with the temperature.
4. The method for measuring the temperature of the sapphire optical fiber in the liquid metal based on the ultrasonic principle as claimed in claim 1, wherein: the number of the radial grooves is two, and a plurality of distributed temperature measuring points are formed.
5. The method for measuring the temperature of the sapphire optical fiber in the liquid metal based on the ultrasonic principle as claimed in claim 1, wherein: the distance between the radial groove position of the temperature measurement sensitive area and the end face of the sapphire optical fiber transmission rod is called as a reflection interval, and when the length of the reflection interval is selected, the following relational expression is satisfied:
in the formula: Δ L — reflection spacing; t is t1-ultrasonic pulse excitation time; v (T) -the ultrasonic wave velocity; Δ t — time difference.
6. The method for measuring the temperature of the sapphire optical fiber in the liquid metal based on the ultrasonic principle as claimed in claim 1, wherein: the sound velocity values of the sapphire optical fiber propagation rod at different temperatures from normal temperature to high temperature are obtained by obtaining a time delay data graph at normal temperature to 1600 ℃ and calculating to obtain a relation curve of the temperature and the time delay data. And during actual application, calculating the speed according to the obtained delay data according to v ═ 2l/t, and searching a relation curve of the temperature and the sound velocity to further obtain the actual temperature.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201910976150.9A CN110686795A (en) | 2019-10-15 | 2019-10-15 | Temperature measurement method of sapphire optical fiber in liquid metal based on ultrasonic principle |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201910976150.9A CN110686795A (en) | 2019-10-15 | 2019-10-15 | Temperature measurement method of sapphire optical fiber in liquid metal based on ultrasonic principle |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CN110686795A true CN110686795A (en) | 2020-01-14 |
Family
ID=69112604
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201910976150.9A Pending CN110686795A (en) | 2019-10-15 | 2019-10-15 | Temperature measurement method of sapphire optical fiber in liquid metal based on ultrasonic principle |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN110686795A (en) |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN108279078A (en) * | 2018-03-20 | 2018-07-13 | 中国计量大学 | Noninvasive temperature estimation device based on pyroelectric effect |
-
2019
- 2019-10-15 CN CN201910976150.9A patent/CN110686795A/en active Pending
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN108279078A (en) * | 2018-03-20 | 2018-07-13 | 中国计量大学 | Noninvasive temperature estimation device based on pyroelectric effect |
Non-Patent Citations (2)
| Title |
|---|
| 原东方 等: "基于超声波的蓝宝石温度传感器", 《科学技术与工程》 * |
| 王凯 等: "蓝宝石超声导波原理的温度分布传感器", 《研究与开发》 * |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN101343676B (en) | On-line detecting device and method for temperature of blast furnace chamber | |
| US20160320324A1 (en) | Method for Predicting the Life of Transformer based on Fiber Grating Temperature Measurement System | |
| CN101571428A (en) | Multi-function sensor and heat current and temperature measuring method under high temperature | |
| CN103487165B (en) | Explosive fusion cast process process internal Temperature Distribution test macro | |
| CN105486424A (en) | Ultrasonic non-invasive measurement method for transient temperature field of inner wall of combustion chamber | |
| Liang et al. | Research and implementation of a 1800° C sapphire ultrasonic thermometer | |
| CN110686794A (en) | Sapphire optical fiber temperature measuring device based on ultrasonic principle | |
| JP2015230171A (en) | Temperature measurement method of lightning protection element in arrester constituted of lightning protection element and porcelain tube covering the same | |
| CN111879443A (en) | Tool for measuring density of gas-liquid two-phase heat flow in rocket engine | |
| CN109324079B (en) | Material thermal expansion coefficient measuring method based on ultrasound | |
| CN104697665A (en) | Distributed optical fiber-based blast furnace hot blast stove temperature monitoring system and method | |
| CN105675161A (en) | Method for measuring temperature of laser processing workpiece via thermocouple | |
| CN110686795A (en) | Temperature measurement method of sapphire optical fiber in liquid metal based on ultrasonic principle | |
| CN203455295U (en) | Phase-transition temperature tester | |
| CN203519207U (en) | Heat flux sensor | |
| CN110146550B (en) | Method for monitoring oxidation degree of composite material high-temperature part based on electrical impedance imaging | |
| CN201220947Y (en) | On-line detecting method for temperature of blast furnace chamber | |
| CN107966472B (en) | Nondestructive rapid measurement method for high-temperature contact thermal resistance | |
| CN105403323B (en) | A kind of inside configuration temperature field measurement method based on phase-detection | |
| CN205679319U (en) | Metal material surface dynamic temperature point based on reflectance change measures system | |
| CN103353466A (en) | Measuring method for heat flux density of solid metal | |
| CN103884448A (en) | Inbuilt type X-ray imaging method and device for measuring temperature in member | |
| CN109506807B (en) | Method for simultaneously measuring internal temperature and wall thickness of high-temperature structure under steady-state condition | |
| CN201983875U (en) | Multi-point temperature measurement probe with low damage and accurate location | |
| Wei et al. | A measurement system of high-temperature oxidation environment with ultrasonic Ir0. 6Rth0. 4 alloy thermometry |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PB01 | Publication | ||
| PB01 | Publication | ||
| SE01 | Entry into force of request for substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| WD01 | Invention patent application deemed withdrawn after publication | ||
| WD01 | Invention patent application deemed withdrawn after publication |
Application publication date: 20200114 |