CN108614005A - A kind of test method and system of the thermal physical property parameter based on multilayer materials - Google Patents

A kind of test method and system of the thermal physical property parameter based on multilayer materials Download PDF

Info

Publication number
CN108614005A
CN108614005A CN201810330613.XA CN201810330613A CN108614005A CN 108614005 A CN108614005 A CN 108614005A CN 201810330613 A CN201810330613 A CN 201810330613A CN 108614005 A CN108614005 A CN 108614005A
Authority
CN
China
Prior art keywords
thermal
physical property
multilayer materials
property parameter
thermal physical
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.)
Granted
Application number
CN201810330613.XA
Other languages
Chinese (zh)
Other versions
CN108614005B (en
Inventor
祝渊
段淇耀
孙琪
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Jieyao Precision Hardware Shenzhen Co ltd
Original Assignee
Southwest University of Science and Technology
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Southwest University of Science and Technology filed Critical Southwest University of Science and Technology
Priority to CN201810330613.XA priority Critical patent/CN108614005B/en
Publication of CN108614005A publication Critical patent/CN108614005A/en
Application granted granted Critical
Publication of CN108614005B publication Critical patent/CN108614005B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N25/00Investigating or analyzing materials by the use of thermal means
    • G01N25/20Investigating or analyzing materials by the use of thermal means by investigating the development of heat, i.e. calorimetry, e.g. by measuring specific heat, by measuring thermal conductivity
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N25/00Investigating or analyzing materials by the use of thermal means
    • G01N25/18Investigating or analyzing materials by the use of thermal means by investigating thermal conductivity

Abstract

The invention discloses a kind of test methods of the thermal physical property parameter based on multilayer materials comprising following steps:System is tested object heating to multilayer materials, and measures tested object temperatur-timel curve T (t);System-computed obtains the thermal resistance and interface resistance that the multilayer materials are tested object vertical direction layers of material;System carries out analogue simulation, and the heat biography obtained between layers of material is disturbed;System measures plane thermal physical property parameter using Angstrom methods, and is converted to related thermal physical property parameter.A kind of test system of the thermal physical property parameter based on multilayer materials comprising:Temperatur-timel curve acquisition module, thermal resistance conversion module, system carry out analogue simulation, thermal physical property parameter computing module.By the above-mentioned means, the present invention can measure multilayer materials vertical direction thermal resistance and horizontal direction thermal diffusion coefficient, and simulate the hot crosstalk direction of hot-fluid between multilayer material, material Thermal test field can be widely applied to.

Description

A kind of test method and system of the thermal physical property parameter based on multilayer materials
Technical field
The present invention relates to material Thermal test fields, and in particular to a kind of test method of multilayer materials thermal physical property parameter And system.
Background technology
As multilayer materials are growing, more and more applications are obtained, while with microelectric technique Development, electronic component is to thin, light, small, multifunction direction change, and component packing density is higher and higher, power device Heat dissipation has become an outstanding problem.If the heat of accumulation cannot shed in time, component operating temperature will be caused to increase, directly Connect the life and reliability for influencing various high-precision equipments.Heat-conducting polymer material processing and forming is simple, at low cost, quality Gently, chemical stability is high, is adjusted by being formulated, the heat dissipation composite material met the requirements can be made.Multilayer materials at One ring of key of electronic equipment dissipating heat will be solved the problems, such as future, and how accurately be surveyed after researcher synthesizes composite material It is most important to try out its corresponding thermal physical property parameter.Accurately know thermal physical property parameter and interface resistance of material etc., ability Know whether material property meets the requirements, and then could preferably develop new multilayer materials.
There are hot cross-interference issue between multilayer materials, be because:Multilayer materials and homogenous material performance are less Identical, hot crosstalk mutual between different materials, interface is asymmetric in heat transfer process, between layers heat transfer system The material that number differs greatly, hot crosstalk is more serious, is produced a very large impact to result;It is this deviate it is big when can be more than 10%. Thermometric error more than 10% may derive the error more than 20% in substituting into formula and calculating.Currently, most of heat The theory of testing is all built upon on the basis of One-dimensional heat transfer hypothesis, and the hot cross-interference issue of multilayer materials can not be ignored, therefore It needs new theory or is used after being modified pervious Thermal test theory hypothesis condition and boundary condition.
Therefore presently, the theory of the still unified authority of neither one tests the hot physical property of multilayer materials with method Parameter.It will produce hot crosstalk during the test for multilayer materials, bring very big test error, it is difficult to measure each The problem of layer material thermal physical property parameter, it is necessary to which a kind of new test method is provided.
Invention content
In order to solve the above-mentioned technical problem, the object of the present invention is to provide a kind of heat testing methods, can measure Vertical Square Thermal diffusion coefficient, thermal conductivity etc. in the thermal resistance, thermal conductivity and horizontal direction of layers of material upwards.
The technical solution adopted in the present invention is:
The present invention provides a kind of test method of the thermal physical property parameter based on multilayer materials comprising following steps:
System is tested object heating to multilayer materials, and measures tested object temperatur-timel curve T (t);
System-computed obtains the thermal resistance and interface resistance that the multilayer materials are tested object vertical direction layers of material;
System carries out analogue simulation, and the heat biography obtained between layers of material is disturbed;
System measures plane thermal physical property parameter using Angstrom methods, and is converted to related thermal physical property parameter.
As the improvement of the technical solution, the step system to multilayer materials be tested object heating, and measure by Tester temperatur-timel curve T (t) comprising:Tested object is placed in insulating box, is heated under condition of different temperatures, and Measured object temperature change is measured using sensor.
As the improvement of the technical solution, differential process is carried out to the temperatur-timel curve of measured tested object, according to It is tested physical performance, the corner position of differential curve determines the layering face of each material layer.
As the improvement of the technical solution, the method further includes:System detectio to experiment sensor test result with When simulation results are corresponding, then stop iteration tests, and record relevant parameter.
Further, the method further includes that system compensates test error caused by hot crosstalk.
Further, the method further includes:Gained temperatur-timel curve is converted into time thermal resistance curve, can be indicated For:
Wherein, T0For the initial temperature of measured object;ΔPhFor thermal power.
Further, derivative da/dz of the time thermal resistance curve under logarithmic time is acquired, deconvolution finds out time constant spectrum For:
Wherein, W (z)=exp [z-exp (z)].
Further, electrothermal module is used to use equal-wattage with sinusoidal or cosine manner to measured object heating one end, separately Two points that spacing is q are chosen in one end, if respectively placing dry temperature sensor, and record temperature information, substitute into formula and obtain Thermal diffusion coefficient;
Wherein, q is measurement point spacing, and dt is phase difference, and M is that one of selected point puts amplitude, and N is another point width Value.
On the other hand, the present invention also provides a kind of test system of the thermal physical property parameter based on multilayer materials, packets It includes:
Temperatur-timel curve acquisition module is tested object heating to multilayer materials for executing step system, and surveys Object temperatur-timel curve T (t) must be tested;
The tested object vertical direction of the multilayer materials is calculated for executing step system in thermal resistance conversion module The thermal resistance and interface resistance of layers of material;
System carries out analogue simulation, and the heat biography obtained between layers of material is disturbed;
Thermal physical property parameter computing module is surveyed for executing step system using Angstrom methods
Plane thermal physical property parameter is measured, and is converted to related thermal physical property parameter.
The beneficial effects of the invention are as follows:This programme provides a kind of test method of multilayer materials thermal physical property parameter and is Multilayer materials, are regarded as the system of an entirety, the hot physical property of tested object are calculated by temperature time curve by system The test of parameter, this method measure material temperature rise curve under the premise of not destroying material, and thermal resistance is parsed by mathematical method With the information such as thermal conductivity, nondestructive measurement is realized.It uses Transient Method to measure, and time of measuring is short, strong antijamming capability, once can be with Multiple parameters are measured, it is efficient, the Thermal test of various nonmetal solid materials is can be widely applied to, there is efficient, quick, use The features such as range is wide.
Description of the drawings
The specific implementation mode of the present invention is described further below in conjunction with the accompanying drawings:
Fig. 1 is the step flow chart of first embodiment of the invention;
Fig. 2 is the temperature curve schematic diagram that the Angstrom method sensor measurements of second embodiment of the invention obtain;
Fig. 3 is the Angstrom method experimental method schematic diagrames of third embodiment of the invention.
Specific implementation mode
It should be noted that in the absence of conflict, the features in the embodiments and the embodiments of the present application can phase Mutually combination.
As shown in Figs. 1-3, the present invention provides a kind of test method of the thermal physical property parameter based on multilayer materials, packet Include following steps:
System is tested object heating to multilayer materials, and measures tested object temperatur-timel curve T (t);
System-computed obtains the thermal resistance and interface resistance that the multilayer materials are tested object vertical direction layers of material;
System carries out analogue simulation, and the heat biography obtained between layers of material is disturbed;
System measures plane thermal physical property parameter using Angstrom methods, and is converted to related thermal physical property parameter.
As the improvement of the technical solution, the step system to multilayer materials be tested object heating, and measure by Tester temperatur-timel curve T (t) comprising:Tested object is placed in insulating box, is heated under condition of different temperatures, and Measured object temperature change is measured using sensor.
As the improvement of the technical solution, differential process is carried out to the temperatur-timel curve of measured tested object, according to It is tested physical performance, the corner position of differential curve determines the layering face of each material layer.
As the improvement of the technical solution, the method further includes:System detectio to experiment sensor test result with When simulation results are corresponding, then stop iteration tests, and record relevant parameter.
Further, the method further includes that system compensates test error caused by hot crosstalk.
Further, the method further includes:Gained temperatur-timel curve is converted into time thermal resistance curve, can be indicated For:
Wherein, T0For the initial temperature of measured object;ΔPhFor thermal power.
Further, derivative da/dz of the time thermal resistance curve under logarithmic time is acquired, deconvolution finds out time constant spectrum For:
Wherein, W (z)=exp [z-exp (z)].
Further, electrothermal module is used to use equal-wattage with sinusoidal or cosine manner to measured object heating one end, separately Two points that spacing is q are chosen in one end, if respectively placing dry temperature sensor, and record temperature information, substitute into formula and obtain Thermal diffusion coefficient;
Wherein, q is measurement point spacing, and dt is phase difference, and M is that one of selected point puts amplitude, and N is another point width Value.
A kind of test method of multilayer materials thermal physical property parameter is regarded measurand as a total system, is passed through Curve (output) is changed over time to measuring measured object temperature after tested object heating (input), object temperature is tested by analysis Time graph parses related thermal physical property parameter, including following steps:
(a) temperature time curve for being tested sample is obtained, integral structure function curve is extracted, calculates vertical direction Interface resistance between upper layers of material thermal resistance and layers of material;
(b) experimental data base is established through a large number of experiments, and analogue simulation goes out multilayer materials internal heat flows side accordingly To the hot crosstalk between different layers;
(c) current heat testing method is modified according to the result of emulation, multilayer is measured using Angstrom methods Composite material plane thermal diffusivity is converted into the parameters such as thermal resistance, thermal conductivity according to physical relation.
It is specifically included:Tested object is placed in insulating box, is heated under condition of different temperatures and is tested object, and used Sensor obtains measured object temperature rising curve.
According to the distributed data of temperature at any time on the heat flow path, be converted on heat source to heat flow path at each point Accumulation thermal capacitance with the delta data of accumulation thermal resistance, i.e. the thermal resistance structure function of measurand, including integral structure function and micro- Separation structure function.
Differential process is carried out to the temperature time curve of measured tested object, according to tested physical performance, differential curve Inflection point determine material layer.
During extracting differential and integral structure function, specific filter and its scope of application are selected.
According to measured vertical direction parameter, carries out the hot crosstalk of multilayer material using computer software and simulate, mould is set Parameter during quasi-.
In conjunction with the hot cross-talk models for the multilayer material that hydrodynamics, thermal conduction study etc. simulate, Binding experiment adjusts emulation ginseng Number.
According to the method that hot cross-talk models compensate and correct the error that hot-fluid crosstalk is brought, Angstrom methods measure more The plane thermal diffusion coefficient of layer material.
Further, first, the temperature time curve for being tested sample is obtained, integral structure function curve is extracted, calculates Go out the interface resistance between layers of material thermal resistance and layers of material in vertical direction;Detected material is placed on thermostat In, temperature is recorded by heating device and changes over time data, while recording the situation of change of heating device voltage, measures measurement The transformational relation of voltage and temperature.Can be in the hope of the temperature value under each time by the expression formula of transformational relation, and then establish A series of temperatur-timel curve, expression formula are as follows:
T (t)=m*V (t)+k;
Wherein, m, k are linear scale factor (being obtained according to experimental result adjustment);V (t) is voltage;T is the time.
Initial temperature T is found out according to above formula0, the reference point of proper range is chosen first on temperatur-timel curve;Then Least squares method calculating is done to the reference point of selection, seeks estimating the Trendline L by these points;Measurement initial stage finally there is into generation The time of obvious errors substitutes into the value of straight line L, can acquire temperature results and initial temperature T after making corrections0
Correction calculating is carried out to the error of above-mentioned temperature-time curve, the initial temperature of measured object is acquired, is considered as line Sexual intercourse, i.e.,:
Wherein, Ph/A represents thermal power densities, is considered as steady state value;Kth is Wherein c is thermal capacitance, and ρ is density, and λ is thermal conductivity.
Thermal resistance-time transformational relation is established according to temperature-time curve, conversion relational expression is:
Wherein T0For initial temperature, Δ P is thermal power change rate.
Regard thermal response as first-order system respond herein, tested object temperature-responsive indicated with the sum of exponential function, I.e.:
Wherein τi=Rthi·Cthi
Assuming that Δ P=1W, temperature-responsive is unit-step response, i.e.,:
Discrete thermal time constant value is composed with continuous thermal time constant and is replaced, can be obtained:
Wherein R (τ) is time constant.
It differentiates to thermal resistance-time graph, its thermal time constant can be acquired by deconvolution, i.e.,:
Each Δ z corresponds to a parallel RC circuits, then corresponding to thermal resistance, thermal capacitance can be expressed as:
Rth=R (z)/Δ z;
Cth=ez/Rth
For the description thermal resistance thermal capacitance information of more intuitive and convenient, being integrated to it can obtain:
Wherein λ is thermal conductivity, and A (x) is cross-sectional area.
Wherein cvIt is unit thermal capacitance, A (x) is cross-sectional area.
By differentiating to thermal resistance-time graph, time constant is sought, integral structure function is converted to, is tied by integrating Structure function parses corresponding thermal resistance, thermal capacitance information;Further according to physical relation conversion can obtain thermal resistance in vertical direction, thermal capacitance and The parameter informations such as thermal conductivity.
Then, experimental data base is established through a large number of experiments, and analogue simulation goes out multilayer materials internal heat flows accordingly Hot crosstalk between direction and different layers;By based on FInite Element, by solve partial differential equation (single physical field) or Person's partial differential equations (multiple physical field) realize the emulation of actual physical phenomenon, simulate multilayer material change of temperature field feelings Condition.
Third walks, and according to the normal direction thermal resistance information parsed, simulation material change of temperature field, is being heated in a computer 10 thermocouple collecting temperature change informations of Shi Caiyong, are compared with computer simulation result, adjustment analogue simulation ginseng Number is allowed to match with experimental result, and simulation parameter iterates if mismatching, until simulation result is passed with practical Sensor measured result stops iteration in error range, records relevant parameter.
4th step is adopted after being compensated and corrected in conjunction with the Thermal test error that simulation result brings the hot crosstalk of multilayer material Multilayer materials plane thermal diffusivity is measured with Angstrom methods, sine is given using electrothermal module in tested object one end Wave heating signal chooses at 2 points on tested object, horizontal direction thermal diffusion coefficient is obtained according to following formula.
Wherein, q is measurement point spacing, and dt is phase difference, and M is that one of selected point puts amplitude, and N is another point width Value.
On the other hand, the present invention also provides a kind of test system of the thermal physical property parameter based on multilayer materials, packets It includes:
Temperatur-timel curve acquisition module heats multilayer materials tester for executing step system, and measures Tested object temperatur-timel curve T (t);
Thermal resistance conversion module, for executing step system, that the multilayer materials tester vertical direction is calculated is each The thermal resistance and interface resistance of layer material;
System carries out analogue simulation, and the heat biography obtained between layers of material is disturbed;
Thermal physical property parameter computing module measures the hot physical property ginseng of plane for executing step system using Angstrom methods Number, and be converted to related thermal physical property parameter.
This programme regards measurand as a total system, by measuring measured object after tested object heating (input) Temperature changes over time curve (output), and being tested object temperature time curve by analysis calculates vertical direction layers of material Interface resistance between thermal resistance and layers of material;Hot crosstalk between different materials is gone out by calculating simulation again, Binding experiment data are true Plane thermal physical property parameter is measured using Angstrom methods after the test error compensation determined analog parameter, and hot crosstalk is brought, It is converted into related thermal physical property parameter further according to physical relation.It hangs down by the above-mentioned means, the present invention can measure multilayer materials Histogram simulates the hot crosstalk direction of hot-fluid between multilayer material to thermal resistance and horizontal direction thermal diffusion coefficient.
It is to be illustrated to the preferable implementation of the present invention, but the invention is not limited to the implementation above Example, those skilled in the art can also make various equivalent variations or be replaced under the premise of without prejudice to spirit of that invention It changes, these equivalent deformations or replacement are all contained in the application claim limited range.

Claims (9)

1. a kind of test method of the thermal physical property parameter based on multilayer materials, which is characterized in that it includes the following steps:
System is tested object heating to multilayer materials, and measures tested object temperatur-timel curve T (t);
System-computed obtains the thermal resistance and interface resistance that the multilayer materials are tested object vertical direction layers of material;
System carries out analogue simulation, and the heat biography obtained between layers of material is disturbed;
System measures plane thermal physical property parameter using Angstrom methods, and is converted to related thermal physical property parameter.
2. the test method of the thermal physical property parameter according to claim 1 based on multilayer materials, which is characterized in that institute It states step system and object heating is tested to multilayer materials, and measure tested object temperatur-timel curve T (t) comprising:It will Tested object is placed in insulating box, is heated under condition of different temperatures, and measures measured object temperature change using sensor.
3. the test method of the thermal physical property parameter according to claim 1 or 2 based on multilayer materials, feature exist In to the temperatur-timel curve progress differential process of measured tested object, according to the inflection point of tested physical performance, differential curve The layering face of each material layer of location determination.
4. the test method of the thermal physical property parameter according to claim 3 based on multilayer materials, which is characterized in that institute The method of stating further includes:When the test result of system detectio to experiment sensor is corresponding with simulation results, then stop iteration Test, and record relevant parameter.
5. the test method of the thermal physical property parameter according to claim 4 based on multilayer materials, which is characterized in that institute The method of stating further includes that system compensates test error caused by hot crosstalk.
6. the test method of the thermal physical property parameter according to claim 5 based on multilayer materials, which is characterized in that institute The method of stating further includes:Gained temperatur-timel curve is converted into time thermal resistance curve, is represented by:
Wherein, T0For the initial temperature of measured object;ΔPhFor thermal power.
7. the test method of the thermal physical property parameter according to claim 6 based on multilayer materials, which is characterized in that ask Derivative da/dz of the time thermal resistance curve under logarithmic time is obtained, deconvolution finds out time constant spectrum and is:
Wherein, W (z)=exp [z-exp (z)].
8. the test method of the thermal physical property parameter according to claim 7 based on multilayer materials, which is characterized in that adopt Use equal-wattage with sinusoidal or cosine manner to measured object heating one end with electrothermal module, the other end chooses two that spacing is q It is a, if respectively placing dry temperature sensor, and temperature information is recorded, substitutes into formula and obtain thermal diffusion coefficient;
Wherein, q is measurement point spacing, and dt is phase difference, and M is that one of selected point puts amplitude, and N is another point amplitude.
9. a kind of test system of the thermal physical property parameter based on multilayer materials, which is characterized in that it includes:
Temperatur-timel curve acquisition module, for execute step system to multilayer materials be tested object heating, and measure by Tester temperatur-timel curve T (t);
Each layer of the tested object vertical direction of the multilayer materials is calculated for executing step system in thermal resistance conversion module The thermal resistance and interface resistance of material;
System carries out analogue simulation, and the heat biography obtained between layers of material is disturbed;
Thermal physical property parameter computing module measures plane thermal physical property parameter for executing step system using Angstrom methods, and Be converted to related thermal physical property parameter.
CN201810330613.XA 2018-04-13 2018-04-13 Method and system for testing thermophysical property parameters based on multilayer composite material Active CN108614005B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201810330613.XA CN108614005B (en) 2018-04-13 2018-04-13 Method and system for testing thermophysical property parameters based on multilayer composite material

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201810330613.XA CN108614005B (en) 2018-04-13 2018-04-13 Method and system for testing thermophysical property parameters based on multilayer composite material

Publications (2)

Publication Number Publication Date
CN108614005A true CN108614005A (en) 2018-10-02
CN108614005B CN108614005B (en) 2021-09-21

Family

ID=63660138

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201810330613.XA Active CN108614005B (en) 2018-04-13 2018-04-13 Method and system for testing thermophysical property parameters based on multilayer composite material

Country Status (1)

Country Link
CN (1) CN108614005B (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110261427A (en) * 2019-07-04 2019-09-20 西安交通大学 Multilayer materials thermal conductivity measurement method based on conjugate gradient method
CN110501380A (en) * 2019-07-26 2019-11-26 北京工业大学 A kind of method of layer-by-layer passage measurement multilayer material thermal resistance
CN111610224A (en) * 2020-06-09 2020-09-01 西南科技大学 Data processing method for transient measurement of thermophysical properties of material by hot-wire method
CN111709162A (en) * 2020-04-28 2020-09-25 全球能源互联网研究院有限公司 Method and device for calculating thermal resistance distribution in power semiconductor module and storage medium
CN111965212A (en) * 2020-07-31 2020-11-20 南方科技大学 Thermophysical property calculation method, thermophysical property test system, electronic device, and storage medium
CN112305020A (en) * 2020-11-25 2021-02-02 西北工业大学 Thermal diffusion coefficient measuring device and method
CN112415043A (en) * 2020-10-14 2021-02-26 南方科技大学 Method and device for measuring multilayer composite material
CN116593853A (en) * 2023-05-19 2023-08-15 浙江大学 Simple measurement method for extracting thermal characteristic parameters of transistor device

Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4350446A (en) * 1980-11-03 1982-09-21 E. I. Du Pont De Nemours And Company Method and apparatus for calorimetric differential thermal analysis
CN102142517A (en) * 2010-12-17 2011-08-03 华中科技大学 Multiple-layer phase-change material with low thermal conductivity
RU123161U1 (en) * 2011-12-28 2012-12-20 Федеральное государственное бюджетное образовательное учреждение высшего профессионального образования "Поволжский государственный технологический университет" DEVICE FOR DETERMINING THERMOPHYSICAL QUALITIES OF HEATED CONCRETE BY TEMPERATURE CONDUCTIVITY IN NATURAL CONDITIONS
CN104155336A (en) * 2014-07-17 2014-11-19 清华大学 Method and system for simultaneously measuring heat conductivity, heat diffusivity and heat capacity of low-dimensional material
CN104716109A (en) * 2013-12-11 2015-06-17 台湾积体电路制造股份有限公司 Packages with Thermal Management Features for Reduced Thermal Crosstalk and Methods of Forming Same
US20150300856A1 (en) * 2012-10-19 2015-10-22 Endress+Hauser Flowtec Ag Thermal, Flow Measuring Device
US20160153922A1 (en) * 2014-11-27 2016-06-02 Mediatek Inc. System and method for adaptive thermal analysis
CN106934099A (en) * 2017-02-10 2017-07-07 华南理工大学 A kind of method for determining strain clamp current-carrying capacity and distribution of three-dimensional temperature
JP2017162207A (en) * 2016-03-09 2017-09-14 富士通株式会社 Heat conductivity calculation program, heat conductivity calculation method, and information processing device

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4350446A (en) * 1980-11-03 1982-09-21 E. I. Du Pont De Nemours And Company Method and apparatus for calorimetric differential thermal analysis
CN102142517A (en) * 2010-12-17 2011-08-03 华中科技大学 Multiple-layer phase-change material with low thermal conductivity
RU123161U1 (en) * 2011-12-28 2012-12-20 Федеральное государственное бюджетное образовательное учреждение высшего профессионального образования "Поволжский государственный технологический университет" DEVICE FOR DETERMINING THERMOPHYSICAL QUALITIES OF HEATED CONCRETE BY TEMPERATURE CONDUCTIVITY IN NATURAL CONDITIONS
US20150300856A1 (en) * 2012-10-19 2015-10-22 Endress+Hauser Flowtec Ag Thermal, Flow Measuring Device
CN104716109A (en) * 2013-12-11 2015-06-17 台湾积体电路制造股份有限公司 Packages with Thermal Management Features for Reduced Thermal Crosstalk and Methods of Forming Same
CN104155336A (en) * 2014-07-17 2014-11-19 清华大学 Method and system for simultaneously measuring heat conductivity, heat diffusivity and heat capacity of low-dimensional material
US20160153922A1 (en) * 2014-11-27 2016-06-02 Mediatek Inc. System and method for adaptive thermal analysis
JP2017162207A (en) * 2016-03-09 2017-09-14 富士通株式会社 Heat conductivity calculation program, heat conductivity calculation method, and information processing device
CN106934099A (en) * 2017-02-10 2017-07-07 华南理工大学 A kind of method for determining strain clamp current-carrying capacity and distribution of three-dimensional temperature

Non-Patent Citations (7)

* Cited by examiner, † Cited by third party
Title
A.BYBI ET AL.: "Electrical method for crosstalk cancellation in transducer arrays", 《NDT&E INTERNATIONAL》 *
DONGLIANG ZHAO ET AL.: "Measurement Techniques for Thermal Conductivity and Interfacial Thermal Conductance of Bulk and Thin Film Materials", 《JOURNAL OF ELECTRONIC PACKAGING》 *
JUNQIANGSUN ET AL.: "Long-term drift induced by the electronic crosstalk in Terra MODIS Band 29", 《JOURNAL OF GEOPHYSICAL RESEARCH:ATMOSPHERES》 *
XUE-JUN YAN ET AL.: "Reduce thermal conductivity by forming a nano-phononic crystal on a Si slab", 《A LETTERS JOURNAL EXPLORING THE FRONTIERS PHYSICS》 *
YUAN ZHU: "Heat-loss modified Angstrom method for simultaneous measurements of thermal diffusivity and conductivity of graphite sheets: The origins of heat loss in Angstrom method", 《INTERNATIONAL JOURNAL OF HEAT AND MASS TRANSFER》 *
朱露: "界面热阻测试系统", 《万方学位论文》 *
湛利华 等: "界面接触热阻影响因素的实验研究", 《轻合金加工技术》 *

Cited By (14)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110261427A (en) * 2019-07-04 2019-09-20 西安交通大学 Multilayer materials thermal conductivity measurement method based on conjugate gradient method
CN110501380B (en) * 2019-07-26 2022-03-15 北京工业大学 Method for measuring thermal resistance of multilayer material by layer-by-layer moving
CN110501380A (en) * 2019-07-26 2019-11-26 北京工业大学 A kind of method of layer-by-layer passage measurement multilayer material thermal resistance
CN111709162B (en) * 2020-04-28 2023-05-02 全球能源互联网研究院有限公司 Thermal resistance distribution calculation method and device in power semiconductor module and storage medium
CN111709162A (en) * 2020-04-28 2020-09-25 全球能源互联网研究院有限公司 Method and device for calculating thermal resistance distribution in power semiconductor module and storage medium
CN111610224B (en) * 2020-06-09 2022-06-03 西南科技大学 Data processing method for transient measurement of thermophysical properties of material by hot-wire method
CN111610224A (en) * 2020-06-09 2020-09-01 西南科技大学 Data processing method for transient measurement of thermophysical properties of material by hot-wire method
CN111965212A (en) * 2020-07-31 2020-11-20 南方科技大学 Thermophysical property calculation method, thermophysical property test system, electronic device, and storage medium
CN111965212B (en) * 2020-07-31 2023-05-09 捷耀精密五金(深圳)有限公司 Thermophysical property calculation method, thermophysical property test system, electronic device, and storage medium
CN112415043A (en) * 2020-10-14 2021-02-26 南方科技大学 Method and device for measuring multilayer composite material
CN112305020B (en) * 2020-11-25 2021-10-01 西北工业大学 Thermal diffusion coefficient measuring device and method
CN112305020A (en) * 2020-11-25 2021-02-02 西北工业大学 Thermal diffusion coefficient measuring device and method
CN116593853A (en) * 2023-05-19 2023-08-15 浙江大学 Simple measurement method for extracting thermal characteristic parameters of transistor device
CN116593853B (en) * 2023-05-19 2024-03-26 浙江大学 Simple measurement method for extracting thermal characteristic parameters of transistor device

Also Published As

Publication number Publication date
CN108614005B (en) 2021-09-21

Similar Documents

Publication Publication Date Title
CN108614005A (en) A kind of test method and system of the thermal physical property parameter based on multilayer materials
CN101112306B (en) Method and equipment for non-invasive core temperature measuring and the calibration equipment and the calibration method thereof
Mierzwiczak et al. The determination temperature-dependent thermal conductivity as inverse steady heat conduction problem
Schelle et al. Analysis of the Agreement of Soil Hydraulic Properties Obtained from Multistep-Outflow and Evaporation MethodsAll rights reserved. No part of this periodical may be reproduced or transmitted in any form or by any means, electronic or mechanical, including photocopying, recording, or any information storage and retrieval system, without permission in writing from the publisher.
CN104034749B (en) Based on the method for testing of thermal contact resistance between the layer material of 3 ω methods
CN104237299B (en) Measure PDMS, SiO in silicon rubber compound insulator2, ATH content thermal analysis system
Liu et al. Advances in the heat‐pulse technique: Improvements in measuring soil thermal properties
Trautz et al. Sensible heat balance and heat-pulse method applicability to in situ soil-water evaporation
Schwartz et al. Estimating hydraulic properties of a fine‐textured soil using a disc infiltrometer
CN114544699B (en) Method for testing thermal resistance and thermal conductivity coefficient of material
Anis-ur-Rehman et al. A modified transient method for an easy and fast determination of thermal conductivities of conductors and insulators
CN109655485B (en) A method of specific heat of liquid is measured using null method
Cuadrado et al. Non-linear non-Iterative transient inverse conjugate heat transfer method applied to microelectronics
Malinarič Step-wise transient method
Sang et al. Wind effects on soil thermal properties measured by the dual‐probe heat pulse method
CN101843476A (en) Calibration facility of non-invasive core temperature measuring device and use method thereof
Jamroz Relationship between dynamic coefficients of two temperature sensors under nonstationary flow conditions
Gustavsson et al. Thermal effusivity measurements of insulating liquids using microsized hot strip probes
CN102128855B (en) Device and method for measuring high temperature thermophysical property
Vitrac et al. A method for time and spatially resolved measurement of convective heat transfer coefficient (h) in complex flows
Mikkelson Characterization and modeling of the thermal properties of photopolymers for material jetting processes
Shojaeefard et al. The estimation of time-varying thermal contact conductance between two fixed contacting surfaces
Heyd Real-time heat conduction in a self-heated composite slab by Padé filters
CN110261432A (en) Non-embedded multilayer materials thermal coefficient steady state measurement method
Platek et al. An accurate method for thermal conductivity measurement of thermally conductive adhesives

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
GR01 Patent grant
GR01 Patent grant
TR01 Transfer of patent right

Effective date of registration: 20230106

Address after: 518104 Buildings 12, 13, 16, 17, Block A, Gonghe First Industrial Zone, Shajing Street, Bao'an District, Shenzhen City, Guangdong Province

Patentee after: Jieyao Precision Hardware (Shenzhen) Co.,Ltd.

Address before: No. 1088, Xili Xueyuan Avenue, Nanshan District, Shenzhen, Guangdong Province

Patentee before: SOUTH University OF SCIENCE AND TECHNOLOGY OF CHINA

TR01 Transfer of patent right