Irregular blocky solid heat conductivity coefficient measuring device and measuring method thereof
By using a CT detector and a three-dimensional scanner in the thermal conductivity measurement device combined with a genetic algorithm optimization, the error problem caused by the randomness of heating spot selection in the prior art is solved, and the accurate measurement of the thermal conductivity and pore distribution of porous materials is achieved.
Patent Information
- Application Number
- CN202411475701.0
- Authority / Receiving Office
- CN · China
- Patent Type
- Applications(China)
- Current Assignee / Owner
- Filing Date
- 2024-10-22
- Publication Date
- 2024-12-31
- Estimated Expiration
- 2044-10-22
AI Technical Summary
The existing thermal conductivity measurement methods have randomness when selecting heating points, resulting in less obvious temperature rise signal, large errors, and the law between the thermal conductivity coefficient and pore distribution of pore materials cannot be accurately obtained.
Using an irregular block solid thermal conductivity measurement device including CT detector, three-dimensional scanner, computing system, pulse light source system, temperature detection device, rocker arm, rotary stage and rotary guide rail, the best results are obtained through three-dimensional scanning and genetic algorithm optimization. The light source incident position and temperature measurement point are used to establish a transient thermal diffusion model to measure thermal conductivity.
Through three-dimensional scanning and genetic algorithm optimization, the measurement error problem in traditional methods is solved, the thermal conductivity coefficient of the opposite-sex material is accurately obtained, and the pore distribution of porous materials can be effectively analyzed.
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Figure CN119224044A_ABST
Abstract
Description
Technical Field
[0001] The invention belongs to the technical field of irregular block solid thermal conductivity measurement, and in particular relates to an irregular block solid thermal conductivity measurement device and a measurement method thereof. Background Art
[0002] Thermal conductivity is one of the basic parameters for measuring the thermal properties of an object. Heterogeneous bulk materials are commonly found in aerospace, oil extraction, rock excavation, geothermal development, frozen soil engineering and other related fields. Accurate thermal conductivity measurement can better analyze the evolution history of rocks, the cyclic characteristics of frozen soil, and simulate the distribution characteristics of the temperature field around rocks and soil during oil extraction to provide thermal protection. Therefore, accurate and efficient measurement of the thermal conductivity of heterogeneous bulk materials has important practical and theoretical significance.
[0003] The measurement of thermal conductivity can be generally divided into steady-state method and non-steady-state method. In the steady-state method, the sample to be tested is compressed into a standardized material plate, and the thermal conductivity is calculated using a balanced heat flux meter under a constant temperature gradient. Since the material needs to be changed into a standard shape, this type of measurement is destructive and cannot be applied to porous materials. For the non-steady-state method, thermal scanning and line source technology are two commonly used methods. The heat source and thermal sensor are moved at the same speed and kept at a constant distance from each other. The thermal conductivity is obtained by measuring the change in the temperature signal of the thermal sensor with distance. This type of method usually takes a long time to measure, and for materials with low thermal conductivity, the temperature signal of the thermal sensor is weak, which will cause large errors.
[0004] However, the above-mentioned thermal conductivity measurement method has the following problems to a greater or lesser extent: there is randomness in the selection of heating points, and sometimes the temperature rise signal of the selected measurement point is not obvious, resulting in a large measurement error; for porous materials, it is impossible to accurately obtain the law between its thermal conductivity and pore distribution. Summary of the invention
[0005] In view of this, the present invention aims to propose a device for measuring the thermal conductivity of irregular block solids and a method for measuring the same, so as to solve the problems that the existing measuring devices have randomness in selecting heating points, sometimes the temperature rise signal of the selected measuring point is not obvious, resulting in large measurement errors, and for porous materials, the law between their thermal conductivity and pore distribution cannot be accurately obtained.
[0006] To achieve the above object, the present invention adopts the following technical solutions:
[0007] A device for measuring thermal conductivity of irregular block solids, comprising a CT detector, a three-dimensional scanner, a computing system, a pulse light source system, a temperature detection device, a rocker arm, a turntable, a rotating guide rail and a horizontal moving mechanism, wherein the horizontal moving mechanism is arranged on a test bench, the turntable is mounted on the horizontal moving mechanism, the three-dimensional scanner is mounted on the side of the horizontal moving mechanism, the CT detector is located above one end of the horizontal moving mechanism and is mounted on the test bench, the rotating guide rail is mounted on the other end of the horizontal moving mechanism, the temperature detection device is mounted on the rotating guide rail, the rocker arm is mounted on the test bench and is arranged in close contact with the side of the horizontal moving mechanism, the pulse light source system is mounted on the rocker arm, the CT detector, the three-dimensional scanner, the pulse light source system, the temperature detection device, the rocker arm, the turntable, the rotating guide rail and the horizontal moving mechanism are all connected to the computing system through a control line, and a sample to be detected is placed on the turntable.
[0008] Furthermore, the horizontal moving mechanism includes a moving guide rail and a moving slider, the moving slider is slidably mounted on the moving guide rail, the moving guide rail is mounted on the test bench, and the turntable is mounted on the moving slider.
[0009] Furthermore, the control modules of the movable guide rail and the turntable are connected to the computing system via control lines.
[0010] Furthermore, the control modules of the rotating guide rail and the rocker arm are connected to the computing system via control lines.
[0011] Furthermore, the scanning direction of the three-dimensional scanner is facing the sample to be inspected.
[0012] A method for measuring thermal conductivity of an irregular block solid, comprising the following steps:
[0013] Step 1: Place the sample to be tested on the turntable;
[0014] Step 2: Move the sample to be tested to the detection area of the 3D scanner by moving the slider, and scan it with the 3D scanner;
[0015] Step 3: Determine whether the computing system obtains a three-dimensional scanning signal;
[0016] Step 4: After obtaining the three-dimensional scanning signal, the slider is moved to the detection area of the CT detector by moving the slider, and detection is performed by the CT detector;
[0017] Step 5: Determine whether the computing system obtains the signal of the CT detector;
[0018] Step 6: After obtaining the signal of the CT detector, the computing system calculates the optimal incident position of the light source of the pulse light source system and the optimal detection position of the temperature detection device;
[0019] Step 7: Then control the turntable, rocker arm and rotating guide rail to move to corresponding positions respectively;
[0020] Step 8: The pulse light source system emits energy, and the temperature detection device detects and transmits the temperature rise information to the computing system;
[0021] Step 9: The computing system performs data analysis to obtain the thermal conductivity.
[0022] Furthermore, if no three-dimensional scanning signal is obtained in step 3, scanning needs to be performed again using a three-dimensional scanner.
[0023] Furthermore, the signal not obtained from the CT detector in step 5 needs to be detected again by the CT detector.
[0024] Furthermore, in step 6, the computing system optimizes and calculates the best incident position of the light source of the pulse light source system and the best detection position of the temperature detection device through a genetic algorithm.
[0025] Compared with the prior art, the present invention has the following beneficial effects:
[0026] 1. The present invention can obtain the three-dimensional morphology of the sample to be detected by collecting images with a three-dimensional scanner and controlling the rotation of the sample to be detected above the turntable by a computing system.
[0027] 2. The present invention can obtain the internal defects of the sample to be tested through the CT detector.
[0028] 3. The present invention obtains an irregular three-dimensional structure with pores in the form of nodes and node connections through a CT detector, takes the best incident point and the best measurement point as optimization variables, and uses a genetic algorithm to optimize the best incident point and the best measurement point as the goal of the best thermal response.
[0029] 3. The present invention combines the surface morphology obtained by a three-dimensional scanner with the internal defects obtained by a CT detector to obtain the three-dimensional structure of the sample to be tested, and transmits the data into a computing system. The computing system converts the imported three-dimensional structure into a data format of nodes and node connections, and optimizes and calculates the best light source position and temperature measurement position through a genetic algorithm, thereby solving the problem of large measurement errors caused by the unclear temperature rise signal due to the randomness of line selection in the traditional heat source method.
[0030] 4. The present invention optimizes the best light source incident point and temperature measurement point of the device through genetic algorithm, establishes a transient thermal diffusion model to measure the temperature difference between the heat source excitation point and the temperature measurement under constant heat flux density boundary conditions, and inverts the thermal conductivity of the heterogeneous material. BRIEF DESCRIPTION OF THE DRAWINGS
[0031] The accompanying drawings constituting a part of the present invention are used to provide a further understanding of the present invention. The exemplary embodiments of the present invention and their descriptions are used to explain the present invention and do not constitute an improper limitation of the present invention. In the accompanying drawings:
[0032] Figure 1 This is a schematic structural diagram of a device for measuring thermal conductivity of irregular block solids according to the present invention;
[0033] Figure 2 The present invention provides a measurement flow chart of a device for measuring thermal conductivity of irregular block solids.
[0034] 1-CT detector, 2-3D scanner, 3-computing system, 4-pulse light source system, 5-temperature detection device, 6-rocker arm, 7-turntable, 8-rotating guide rail, 9-moving guide rail, 9-1: moving slider, 10-sample to be tested. DETAILED DESCRIPTION
[0035] The following will be combined with the drawings in the embodiments of the present invention to clearly and completely explain the technical solutions in the embodiments of the present invention. It should be noted that the embodiments of the present invention and the features in the embodiments can be combined with each other without conflict, and the described embodiments are only part of the embodiments of the present invention, not all of the embodiments.
[0036] See also Figure 1-2 The present embodiment is described, a device for measuring thermal conductivity of irregular block solids, comprising a CT detector 1, a three-dimensional scanner 2, a computing system 3, a pulse light source system 4, a temperature detection device 5, a rocker arm 6, a turntable 7, a rotating guide rail 8 and a horizontal moving mechanism, wherein the horizontal moving mechanism is arranged on a test bench, the turntable 7 is mounted on the horizontal moving mechanism, the three-dimensional scanner 2 is mounted on the side of the horizontal moving mechanism, the CT detector 1 is located above one end of the horizontal moving mechanism and is mounted on the test bench, the rotating guide rail 8 is mounted on the other end of the horizontal moving mechanism, the temperature detection device 5 is mounted on the rotating guide rail 8, the rocker arm 6 is mounted on the test bench and is arranged in close contact with the side of the horizontal moving mechanism, the pulse light source system 4 is mounted on the rocker arm 6, the CT detector 1, the three-dimensional scanner 2, the pulse light source system 4, the temperature detection device 5, the rocker arm 6, the turntable 7, the rotating guide rail 8 and the horizontal moving mechanism are all connected to the computing system 3 through a control line, and a sample 10 to be detected is placed on the turntable 7.
[0037] The horizontal moving mechanism includes a moving guide rail 9 and a moving slider 9 - 1 . The moving slider 9 - 1 is slidably mounted on the moving guide rail 9 . The moving guide rail 9 is mounted on the test bench. The turntable 7 is mounted on the moving slider 9 - 1 .
[0038] The control modules of the movable guide rail 9 and the turntable 7 are connected to the computing system 3 via control lines.
[0039] The control modules of the rotating guide rail 8 and the rocker arm 6 are connected to the computing system 3 via control lines.
[0040] The scanning direction of the three-dimensional scanner 2 is facing the sample 10 to be inspected.
[0041] The three-dimensional scanner 2 is fixed on the side of the moving guide rail 9 of the experimental table, and its scanning direction is facing the sample on the turntable 7. The control system of the three-dimensional scanner 2 is connected to the computing system. The computing system 3 controls the rotation of the sample 10 to be tested on the turntable 7 and the image acquisition of the three-dimensional scanner 2 to obtain the three-dimensional morphology of the heterogeneous solid material to be tested. The CT detector 1 is fixed on the experimental table so that the moving guide rail 9 completely passes through the detection area of the CT detector 1. The control system is connected to the computing system 3. The moving guide rail 9 is controlled by the computing system 3 so that the sample 10 to be tested can move back and forth in the detection area. At the same time, the computing system 3 controls the moving guide rail 9. The CT detector 1 issues a sampling instruction to obtain the internal defects of the sample 10 to be tested. The rotating guide rail 8 is fixed on the test bench at the other end of the moving guide rail 9. The temperature detection device 5 is fixed on the rotating guide rail 8. The control systems of the rotating guide rail 8 and the temperature detection device 5 are simultaneously connected to the computing system 3, and the computing system 3 accurately controls the position of the temperature detection device 5. The rocker arm 6 is fixed on the test bench close to the moving guide rail 9. At the same time, the pulse light source system 4 is fixed on the rocker arm 6. The control system of the rocker arm 6 and the control system of the pulse light source system 4 are simultaneously connected to the computing system 3, and the computing system accurately controls the position of the excitation heat source.
[0042] A sample 10 to be tested is placed on the turntable 7, and the sample 10 to be tested is moved to the detection area of the three-dimensional scanner 2 by moving the slider 9-1. The three-dimensional scanner 2 is used to scan and determine whether the computing system 3 obtains a three-dimensional scanning signal. After obtaining the three-dimensional scanning signal, the movable slider 9-1 is moved to the detection area of the CT detector 1 by moving the slider 9-1. The CT detector 1 is used to detect and determine whether the computing system 3 obtains the signal of the CT detector 1. After obtaining the signal of the CT detector 1, the computing system 3 calculates the optimal incident position of the light source of the pulse light source system 4 and the optimal detection position of the temperature detection device 5, and then controls the turntable 7, the rocker arm 6 and the rotating guide rail 8 to move to corresponding positions respectively, the pulse light source system 4 emits energy, the temperature detection device 5 detects and transmits the temperature rise information to the computing system 3, and the computing system 3 performs data analysis to obtain the thermal conductivity.
[0043] The device combines the surface morphology obtained by the three-dimensional scanner 2 with the internal defects obtained by the CT detector 1 to obtain the three-dimensional structure of the sample to be tested, and transmits the data to the computing system 3. The computing system 3 optimizes and calculates the best light source position and temperature measurement position through the genetic algorithm to solve the problem of large measurement errors caused by the unclear temperature rise signal due to the randomness of line selection in the traditional heat source method. The best light source incident point and temperature measurement point of the device are optimized through the genetic algorithm, and a transient thermal diffusion model is established to measure the temperature difference between the heat source excitation point and the temperature measurement under the boundary condition of constant heat flux density, and the thermal conductivity of the heterogeneous material is obtained by inversion.
[0044] A method for measuring thermal conductivity of an irregular block solid, comprising the following steps:
[0045] Step 1: Place the sample 10 to be tested on the turntable 7;
[0046] Step 2: Move the sample 10 to be tested to the detection area of the three-dimensional scanner 2 by moving the slider 9 - 1 and scan it by the three-dimensional scanner 2 ;
[0047] Step 3: Determine whether the computing system 3 obtains a three-dimensional scanning signal. If no three-dimensional scanning signal is obtained, the three-dimensional scanner 2 needs to be used to scan again.
[0048] Step 4: After obtaining the three-dimensional scanning signal, the movable slider 9 - 1 is moved to the detection area of the CT detector 1 by the movable slider 9 - 1 , and detection is performed by the CT detector 1 ;
[0049] Step 5: Determine whether the computing system 3 obtains the signal of the CT detector 1. If the signal of the CT detector 1 is not obtained, the CT detector 1 needs to be used for detection again;
[0050] Step 6: After obtaining the signal from the CT detector 1, the computing system 3 calculates the optimal incident position of the light source of the pulse light source system 4 and the optimal detection position of the temperature detection device 5;
[0051] Step 7: Then control the turntable 7, the rocker arm 6 and the rotating guide rail 8 to move to corresponding positions respectively;
[0052] Step 8: The pulse light source system 4 emits energy, and the temperature detection device 5 detects and transmits the temperature rise information to the calculation system 3;
[0053] Step 9: The computing system 3 performs data analysis to obtain the thermal conductivity.
[0054] In step 6, the computing system 3 calculates the best incident position of the light source of the pulse light source system 4 and the best detection position of the temperature detection device 5 through genetic algorithm optimization.
[0055] Create a MATLAB function named code that receives a two-element vector x as input. The main purpose of this function is to use the Java API of COMSOL Multiphysics software to set the parameters of a physical model and run a simulation. It includes the following steps:
[0056] a: Get two integers m and n from the input vector x, which are used to extract specific node coordinates;
[0057] b: Import node data, extract the coordinate values of nodes m and n, create a model using COMSOL's Java API, and set the model's path and labels;
[0058] c: Set model parameters, such as position coordinates x_r, y_r, z_r and x_t, y_t, z_t and other parameters such as laser width, power, radius, etc.
[0059] d: Generate mesh and solver settings;
[0060] e: Set material properties, such as thermal expansion coefficient, specific heat capacity, density and thermal conductivity, set heat sources and relate them to time and space distribution;
[0061] f: Run the mesh generation and solver, extract the maximum value, and calculate the best time.
[0062] In a measurement method for measuring thermal conductivity of an irregular block solid, in step 6, a computing system 3 optimizes and calculates the optimal incident position of a pulse light source system 4 and the optimal detection position of a temperature detection device 5 by using a genetic algorithm, wherein the genetic algorithm optimization calculation includes the following steps:
[0063] (1) Read node coordinate data, import node coordinate data, and store it in the variable nodes;
[0064] (2) Read node connection data, import node connection output, and store it in the variable elements;
[0065] (3) Design parameter limits. Calculate the length L of the data in the node, set the design parameter lb to [1,1], and the upper bound ub to [L,L]. The optimized parameters are searched within these limits.
[0066] (4) Set the options of the genetic algorithm;
[0067] (5) Call the objective function code, pass in two design parameters, output the optimization results, and display the best incident point position number and the best detection point position number.
[0068] The embodiments of the present invention disclosed above are only used to help illustrate the present invention. The embodiments do not describe all the details in detail, nor do they limit the invention to the specific implementation methods described. According to the content of this specification, many modifications and changes can be made. This specification selects and specifically describes these embodiments in order to better explain the principles and practical applications of the present invention, so that those skilled in the art can understand and use the present invention well.
Claims
1. A device for measuring thermal conductivity of irregular block solids, characterized in that: The invention comprises a CT detector (1), a three-dimensional scanner (2), a computing system (3), a pulse light source system (4), a temperature detection device (5), a rocker arm (6), a turntable (7), a rotating guide rail (8) and a horizontal moving mechanism, wherein the horizontal moving mechanism is arranged on a test bench, the turntable (7) is mounted on the horizontal moving mechanism, the three-dimensional scanner (2) is mounted on the side of the horizontal moving mechanism, the CT detector (1) is located above one end of the horizontal moving mechanism and is mounted on the test bench, the rotating guide rail (8) is mounted on the other end of the horizontal moving mechanism, the temperature detection device (5) is mounted on the rotating guide rail (8), the rocker arm (6) is mounted on the test bench and is arranged in close contact with the side of the horizontal moving mechanism, the pulse light source system (4) is mounted on the rocker arm (6), the CT detector (1), the three-dimensional scanner (2), the pulse light source system (4), the temperature detection device (5), the rocker arm (6), the turntable (7), the rotating guide rail (8) and the horizontal moving mechanism are all connected to the computing system (3) via a control line, and a sample (10) to be detected is placed on the turntable (7).
2. The device for measuring thermal conductivity of irregular block solid according to claim 1, characterized in that: The horizontal moving mechanism comprises a moving guide rail (9) and a moving slider (9-1), wherein the moving slider (9-1) is slidably mounted on the moving guide rail (9), the moving guide rail (9) is mounted on a test bench, and the turntable (7) is mounted on the moving slider (9-1).
3. The device for measuring thermal conductivity of irregular block solid according to claim 2, characterized in that: The control modules of the movable guide rail (9) and the turntable (7) are connected to the computing system (3) via control lines.
4. The device for measuring thermal conductivity of irregular block solid according to claim 1, characterized in that: The control modules of the rotating guide rail (8) and the rocker arm (6) are connected to the computing system (3) via control lines.
5. The device for measuring thermal conductivity of irregular block solid according to claim 1, characterized in that: The three-dimensional scanner (2) has a scanning direction facing the sample (10) to be inspected.
6. A method for measuring thermal conductivity of irregular block solids according to any one of claims 1 to 5, characterized in that: It includes the following steps: Step 1: placing a sample to be tested (10) on a turntable (7); Step 2: Move the sample to be tested (10) to the detection area of the three-dimensional scanner (2) by moving the slider (9-1), and scan it with the three-dimensional scanner (2); Step 3: Determine whether the computing system (3) obtains a three-dimensional scanning signal; Step 4: after obtaining the three-dimensional scanning signal, the movable slider (9-1) is moved to the detection area of the CT detector (1) by the movable slider (9-1), and detection is performed by the CT detector (1); Step 5: Determine whether the computing system (3) obtains the signal of the CT detector (1); Step 6: After obtaining the signal of the CT detector (1), the computing system (3) calculates the optimal incident position of the light source of the pulse light source system (4) and the optimal detection position of the temperature detection device (5); Step 7: Then control the turntable (7), the rocker arm (6) and the rotating guide rail (8) to move to corresponding positions respectively; Step 8: The pulse light source system (4) emits energy, and the temperature detection device (5) detects and transmits the temperature rise information to the calculation system (3); Step 9: The computing system (3) performs data analysis to obtain the thermal conductivity.
7. The method for measuring thermal conductivity of an irregular block solid according to claim 6, characterized in that: If no three-dimensional scanning signal is obtained in step 3, scanning needs to be performed again using the three-dimensional scanner (2).
8. The method for measuring thermal conductivity of an irregular block solid according to claim 6, characterized in that: In step 5, the signal of the CT detector (1) that is not obtained needs to be detected again by the CT detector (1).
9. The device for measuring thermal conductivity of irregular block solid according to claim 6, characterized in that: In step 6, the computing system (3) calculates the best incident position of the light source of the pulse light source system (4) and the best detection position of the temperature detection device (5) through the genetic algorithm optimization.
Citation Information
Patent Citations
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CN106768367A
Test device and method for observing rock freeze-thaw damage evolution process and analysis method
CN116990337A
Inversion determination method for heat conductivity coefficient of coal rock matrix
CN118258848A
Method and device for proximate determination of thermal conductivity of solid materials
RU2153664C1