CN102183544A - Thermal-property transient measurement method and device - Google Patents

Thermal-property transient measurement method and device Download PDF

Info

Publication number
CN102183544A
CN102183544A CN 201010590586 CN201010590586A CN102183544A CN 102183544 A CN102183544 A CN 102183544A CN 201010590586 CN201010590586 CN 201010590586 CN 201010590586 A CN201010590586 A CN 201010590586A CN 102183544 A CN102183544 A CN 102183544A
Authority
CN
China
Prior art keywords
temperature
thermal
hot pin
hot
detected materials
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
CN 201010590586
Other languages
Chinese (zh)
Other versions
CN102183544B (en
Inventor
陈昭栋
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to CN201010590586.3A priority Critical patent/CN102183544B/en
Publication of CN102183544A publication Critical patent/CN102183544A/en
Application granted granted Critical
Publication of CN102183544B publication Critical patent/CN102183544B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Investigating Or Analyzing Materials Using Thermal Means (AREA)

Abstract

The invention discloses a thermal-property transient measurement method and device, which are used for automatically measuring thermal conductivity, thermal diffusion coefficient, specific heat at constant pressure and density of a material and are also used for analysing the regular pattern of the thermal property of the material near the room temperature along the change of the temperature. The method comprises the following steps of: placing a cylindrical hot needle in a uniform and infinite medium; and continuously heating the medium by a constant thermal flow through the hot needle to form a one-dimensional cylindrical heat-transferring model in the radical direction. The measurement device comprises a direct-current stable-current power supply, the hot needle, a temperature signal collecting module, a signal processor, a memory and a display. A column body of the hot needle is made of carbon fibre and is composed of a core column and a sleeve pipe; the electric heating element is wounded on the core column through a double-head manganin lacquered wire and the double-head manganin lacquered wire is formed by doubling and winding one manganin lacquered wire along the central point; and an thermoelectric couple is formed by welding one copper wire and one konstantan wire in the thermoelectric couple grade.

Description

Hot rerum natura transient measurement method and device
Technical field
The invention belongs to field of measuring technique, be specifically related to a kind of hot rerum natura transient measurement method and device, be used for measuring automatically thermal conductivity, thermal diffusion coefficient, specific heat at constant pressure and the density of material; Analyze near the temperature variant rule of the hot rerum natura of material of room temperature.
Background technology
The hot rerum natura of material refers to thermal conductivity, thermal diffusion coefficient, specific heat at constant pressure and the density of material.So-called transient state is measured automatically, is in the process of heat temperature raising, finishes work such as automatic measurement, record, deal with data fast.
At home, outward, the 1970s and 1980s in last century, about hot rerum natura instantaneous measurement Study on Technology, a climax was once appearring once.The numerous well-known scholars in home and abroad have made extensive work, have obtained very great achievement.At that time, measuring methods such as impulse method, constant flow method, heat-pole method had been studied.Wherein, these two kinds of transient measurement methods of impulse method and constant flow method, owing to be subjected to placing restrictions on of technical merit at that time, and many condition effect, the home and abroad scholar fails to achieve one's goal and makes actual adaptable surveying instrument.Thereby once Ban Bu corresponding ministerial standard was also thrown aside at present.In long period, in fact this problem is not resolved.Up to the beginning of this century, just to succeed based on the impulse method of the big heat transfer model of one dimension semiinfinite, the instantaneous measurement instrument of constant flow method, quilt is named is the hot rerum natura transient state of SHT-20 automatic measuring instrument.By contrast, though heat-pole method has national standard and instrument supply the market.But heat-pole method still fails to break through the category of steady state measurement, and it also is not a transient measurement method truly, need to be improved and enhanced.
Summary of the invention
Purpose of the present invention provides a kind of brand-new hot rerum natura transient state method for automatic measurement and device (hot rerum natura transient measurement method of pin type and device), measures thermal conductivity, thermal diffusion coefficient, specific heat at constant pressure and the density of material fast; Analyze near the temperature variant rule of the hot rerum natura of material of room temperature.
Technical scheme of the present invention is:
A kind of hot rerum natura transient measurement method based in even, infinitely great medium, is placed a cylindric hot pin, continues heating by hot pin to medium with constant heat flux, forms one dimension face of cylinder heat transfer model radially, and this heat transfer model is characterized by following formula:
Figure BSA00000387323900021
Figure BSA00000387323900022
(1)
Figure BSA00000387323900023
Figure BSA00000387323900024
In the formula:
Figure BSA00000387323900025
In the expression detected materials, the distance of the hot pin of distance axis is the r place, τ=t-t 0Temperature variation in time;
t 0(s) for adding the initial moment of thermal measurement.
T (r, t) (℃) for the hot pin of distance axis in the medium is the r distant place, t temperature constantly;
T (r, t 0) (℃) for the hot pin of distance axis in the medium is the r distant place, add the temperature in the initial moment of thermal measurement;
Figure BSA00000387323900026
Thermal diffusion coefficient for detected materials;
Figure BSA00000387323900027
Density for detected materials;
The quality of the certain detected materials of m (kg) expression;
V (m 3) represent the volume of this certain detected materials;
c pThe specific heat at constant pressure of J/ (kgk) expression detected materials;
The thermal conductivity of λ W/ (mk) expression detected materials;
Figure BSA00000387323900028
Represent the thermal power that hot pin unit length is sent, or claim calorific intensity;
Effective heated length of the hot pin of l (m) expression;
W=I 2The heating power of the hot pin of R (W) expression;
I (A) is by the strength of current of the heating current of hot pin;
The resistance of the hot pin heater of R (Ω);
The above-mentioned pulse cracking of separating problem surely is
Figure BSA00000387323900031
When continuing heating with constant heat flux, i.e. in the time from τ=0 to τ, r place in the test specimen, the temperature rise that the τ time is interior, an integration of available above-mentioned pulse cracking obtains.This integration can be expressed as a straight line equation approx
Figure BSA00000387323900032
In the formula: slope
Figure BSA00000387323900033
Intercept
Figure BSA00000387323900034
Here, C *=1.78115, be integration constant.
Calculate the thermal conductivity and the thermal diffusion coefficient of material:
With measuring in heat time heating time, obtain temperature-time logarithm ordered series of numbers T (r 0, t)~and lnt, make linear fit with young waiter in a wineshop or an inn's rule, calculate the k of the 1st sample, D then has
Thermal conductivity
Figure BSA00000387323900035
Thermal diffusion coefficient
Figure BSA00000387323900036
With corresponding medial temperature
Figure BSA00000387323900037
From i=1, choose j sample in succession.Repeat aforementioned calculation, make up database [λ j, a j, T j].Then, do conic fitting, draw the experimental formula of calculating thermal conductivity and thermal diffusion coefficient with young waiter in a wineshop or an inn's rule
λ(T)=η 01T+η 2T 2 [T 1,T 2] (8)
a(T)=ζ 01T+ζ 2T 2 [T 1,T 2] (9)
Calculate the thermal conductivity and the thermal diffusion coefficient λ of match intermediate value temperature correspondence, a;
Bulk density and specific heat at constant pressure
Density
Figure BSA00000387323900038
Specific heat at constant pressure
Figure BSA00000387323900039
Device based on above-mentioned hot rerum natura transient measurement method, comprise dc current stabilized power supply, hot pin, temperature signal collection module, signal processor, storer, display, described hot pin is cylindric, makes with insulating material, and post contains thermocouple and electrical heating elements; Described storer prestores the computation model of thermal physical property parameter, and described dc current stabilized power supply is powered to temperature collect module.Thermocouple output temperature signal, temperature collect module converts this temperature signal to digital signal, sends into signal processor, and signal processor is handled according to the computation model of thermal physical property parameter, and result is shown by display.
The cylinder of described hot pin is made with carbon fiber, is made of stem stem and sleeve combination, and on stem stem, this double end copper-manganese enameled wire is to form along mid point doubling coiling with a copper-manganese enameled wire to described electrical heating elements with double end copper-manganese enameled wire.Described thermocouple connects with the copper cash of thermocouple level and each root bead of constantan line and forms.
The efficient heat generation length of described hot pin is more than or equal to 40 times of hot pin overall diameters, i.e. l 〉=40d.
Described dc current stabilized power supply output DC stream is accurate adjustable between 0.01-1.0004; In the time of thermal measurement, the fluctuating range of heating current: Δ I≤± 0.001A.
The temperature resolution of described temperature collect module: Δ T≤0.1k; Sample frequency: adjustable continuously between the 0.5-1Hz.
Technique effect of the present invention:
The one dimension face of cylinder heat transfer model that the present invention sets up truly, is accurately described out the heat conducting objective law of medium, has realized by steady state measurement being the instantaneous measurement of real meaning to the instantaneous measurement transition; The measurement mechanism instantaneous measurement takes extremely short, less than 200 seconds, and little interference by environment, the factor that influence is measured is revised easily, the measurement accuracy height, relative error is about 1%.And can measure thermal diffusion coefficient, thermal conductivity, specific heat at constant pressure, density.
Description of drawings
Fig. 1 is the structured flowchart of this measurement mechanism;
Fig. 2 is the hot pin outer tube structure synoptic diagram of this measurement mechanism;
Fig. 3 is the hot pin inner tube structure synoptic diagram of this measurement mechanism.
Embodiment
Ultimate principle of the present invention is based in even, the infinitely great medium, places a hot pin, continues heating by hot pin to medium with constant heat flux, forms one dimension garden cylinder heat transfer model radially, and this heat transfer model is characterized by following formula:
Figure BSA00000387323900051
(1)
Figure BSA00000387323900053
Figure BSA00000387323900054
In the formula:
Figure BSA00000387323900055
In the expression detected materials, the distance of the hot pin of distance axis is the r place, τ=t-t 0Temperature variation in time;
t 0(s) for adding the initial moment of thermal measurement.
T (r, t) (℃) for the hot pin of distance axis in the medium is the r distant place, t temperature constantly;
T (r, t 0) (℃) for the hot pin of distance axis in the medium is the r distant place, add the temperature in the initial moment of thermal measurement;
Figure BSA00000387323900056
Thermal diffusion coefficient for detected materials;
Figure BSA00000387323900057
Density for detected materials;
The quality of the certain detected materials of m (kg) expression;
V (m 3) represent the volume of this certain detected materials;
c pThe specific heat at constant pressure of J/ (kgk) expression detected materials;
The thermal conductivity of λ W/ (mk) expression detected materials;
Figure BSA00000387323900058
Represent the thermal power that hot pin unit length is sent, or claim calorific intensity;
Effective heated length of the hot pin of l (m) expression;
W=I 2The heating power of the hot pin of R (W) expression;
I (A) is by the strength of current of the heating current of hot pin;
The resistance of the hot pin heater of R (Ω);
The above-mentioned pulse cracking of separating problem surely is
When continuing heating with constant heat flux, i.e. in the time from τ=0 to τ, r place in the test specimen, the temperature rise that the τ time is interior, an integration of available above-mentioned pulse cracking obtains.This integration can be expressed as a straight line equation approx
Figure BSA00000387323900061
In the formula: slope
Figure BSA00000387323900062
Intercept
Figure BSA00000387323900063
Here, C *=1.78115, be integration constant.
Calculate the thermal conductivity and the thermal diffusion coefficient of material:
With measuring in heat time heating time, obtain temperature-time logarithm ordered series of numbers T (r 0, t)~and lnt, make linear fit with young waiter in a wineshop or an inn's rule, calculate the k of i sample, D then has
Thermal conductivity
Figure BSA00000387323900064
Thermal diffusion coefficient
With corresponding medial temperature
Figure BSA00000387323900066
From i=1, choose j sample in succession.Repeat aforementioned calculation, make up database [λ j, a j, T j].Then, do conic fitting, draw the experimental formula of calculating thermal conductivity and thermal diffusion coefficient with young waiter in a wineshop or an inn's rule
λ(T)=η 01T+η 2T 2 [T 1,T 2] (8)
a(T)=ζ 01T+ζ 2T 2 [T 1,T 2] (9)
Calculate the thermal conductivity and the thermal diffusion coefficient λ of match intermediate value temperature correspondence, a;
Bulk density and specific heat at constant pressure
Density
Figure BSA00000387323900067
Specific heat at constant pressure
Figure BSA00000387323900068
Referring to Fig. 1: this device is made up of dc current stabilized power supply A, hot pin B, temperature signal collection module C, signal processor D, storer F, display E.Wherein:
Dc current stabilized power supply A: input: 220V, 50Hz civil power; Output: DC current, accurate adjustable between 0.01-1.000A; In the time of thermal measurement, the fluctuating range of heating current: Δ I≤± 0.001A.
Temperature signal collection module C: temperature resolution: Δ T≤0.1k; Sample frequency: adjustable continuously between the 0.5-1Hz.
Manufacture and design hot pin B, this hot pin B is a heating element, is again temperature element.
Basic demand to hot pin B: firm; Wear-resisting wiping; Except that the termination, uniformity of temperature profile in the longitudinal direction; When temperature raise, the resistance variations of heater element was minimum; The material thermal conductivity is good etc.Structure can consider to use the coaxial sleeve structure.Interior pipe is gone up around sufficiently long heating wire, the outer tube uniform temperature; Outer tube outer surface device temperature element is measured the temperature variation of hot pin and detected materials thermal interface.The control length-diameter ratio allows the efficient heat generation length of hot pin more than or equal to 40 times of hot pin overall diameters, and promptly l 〉=40d generally can satisfy one dimension face of cylinder heat transfer model.If measure temperature with thermocouple, point for measuring temperature should be arranged on the mid point of hot pin efficient heat generation length; Make the tinsel that thermocouple is used, diameter is selected 0.05mm for use.
Through experimental study, this hot pin employing heat conduction carbon fiber pipe good, lightweight is made host material, and manganese-copper filament is made exothermic material, and special-purpose copper constantan thermocouple is used for the hot pin of measuring distance axis r t temperature variation constantly at a distance.And press structural formula
Interior pipe: Φ 2.5 (1) * 211 (4+180+27)+Φ 0.12 * 930[884+2 * 23] mm; The carbon fiber rod of the also available φ 25mm of pipe in being somebody's turn to do; Outer tube: [Φ 4 (0.5) * 186 (180+6)+Φ cu0.05 * 135+cusn0.05 * 135] compound composition of mm.
The hot pin of making like this, except that self measuring error that causes of heat absorption that can revise, the measuring error that all the other factors cause is less than 0.2%.
The meaning of outer tube structure formula: with 4 millimeters of external diameters, wall thickness 0.5 milli, long 186 millimeters carbon fiber pipe is made outer tube.In the longitudinal direction, 180 length are used to cover the manganese-copper filament winding, and 6 millimeters are used for fixing hot pin; Aft section is represented 0.05 millimeter of diameter of temperature element, the thermocouple that long 135 millimeters copper cash and constantan line are formed, and mean that point for measuring temperature is positioned at the midpoint of outer tube outer surface.
The meaning of inner tube structure formula: with 2.5 millimeters of external diameters, 1 millimeter of wall thickness, pipe in long 211 millimeters carbon fiber pipe is done.In the longitudinal direction, 4 millimeters of front ends are used to out locating groove; Middle 180 millimeters are used for around manganese-copper filament; 27 millimeters of the other ends, fixedly connected.Aft section represents, with 0.12 millimeter of diameter, long 930 millimeters manganese-copper filament, wherein, 884 millimeters around the zone of 180 millimeters long, and as heater element, all the other 46 millimeters conducts pick out lead-in wire.
Concrete method for making such as Fig. 2, shown in Figure 3: get 2.5 millimeters of external diameters, 1 millimeter of wall thickness, one of long 211 millimeters carbon fiber pipe.One end is opened wide 1 millimeter in diametric(al), dark 4 millimeters ditch is as the usefulness around the manganese-copper filament location.Then, 0.12 millimeter in cut-off footpath, one of long 930 millimeters insulation enamel manganin, doubling is put into locating groove with mid point.By double helical form the two-wire of 442 millimeters long is evenly curled up on 180 millimeters carbon pipe fixingly, make heating element B-1.Wiring is drawn in 23 millimeters remaining conducts.Get 4 millimeters of external diameters, 0.5 millimeter of wall thickness, long 186 millimeters carbon pipes, the interior pipe that coiling is good screws in from the locating groove end, just all exposes up to locating groove.At this moment, coiling just is all covered.Then, stamen of getting the aviation connector takes out, and the manganese-copper filament extension line is connected on the pin binding post.Learn from else's experience again to demarcate and be 0.05 millimeter of the diameter of thermocouple level; each one on long 135 millimeters copper cash and constantan line longitudinally are arranged in outer tube-surface, and an end is drawn outer tube and is connected on the binding post; other end alignment; move the mid point of outer tube heating part to,, weld unnecessary removing; be bonded at outer tube outer surface; make thermocouple B-2, protective seam is coated on the surface, oven dry.Like this, just, made a hot pin.
Measuring process is as follows:
Write data processing software according to above-mentioned heat transfer model.
Be equipped with the transient state self-operated measuring unit, deposit data processing software in storer F; Hot pin B is connected with temperature signal collection module C.
Choose a certain amount of detected materials, measure its volume V, weigh quality m with physical balance.If measuring object raft material is as long as insert hot pin B.If material is limited, need to prepare a bulk containers.The volume of container should be Φ 200 * 184mm at least.Container is filled, and hot pin B inserts bucket central authorities.If detected materials is a massive material, then on material, punch or fluting, in hot pin B patchhole or groove.The diameter of hole or groove and hot pin diameter adapt, and make hot wire surface can be attached to hole wall or cell wall.
Heating current is set for different detected materials, the varying in size of heating current.In general, density is little, and heating current is suitable smaller.For example, heat-insulation material, heating current can be chosen as between 0.1~0.3A; The detected materials that density is big, electric current is suitable big.
After adding the thermal measurement current settings, connect heating current, measure.Temperature signal collection module C sends temperature signal into signal processor D, and signal processor D is according to the computation model treatment temperature signal that is pre-stored in the thermal physical property parameter among the storer F, and result is shown by display E.
Observe the demonstration of temperature time curve, the numeration of measurement data tabulation.After adding thermal measurement and beginning, when having 70 groups of numerations at least, can stop to measure.
More than be to measure the method that contains the hot rerum natura of wet stock.The variation of moisture percentage is bigger to the influence of measuring.The same material of different moisture percentages, the measured value under uniform temp does not have the property of comparison.The hot rerum natura of having only the over dry material, the measured value under same temperature is only consistent.
Measure the hot rerum natura of over dry material, before measuring, need to use electrically heated drying cabinet, detected materials is baked to constant weight repeatedly, be stored in the exsiccator.Treat cool but after, measure again.Only under the over dry condition, the hot rerum natura that measures just has the property compared comparatively accurately.
In order to try to achieve the temperature variant rule of the hot rerum natura of material, can get j=1,2,3, Λ Λ N calculates the [λ (T of N sample in succession j), T j] and [a (T j), T j].Make fitting of a polynomial with young waiter in a wineshop or an inn's rule, the experimental formula that can change with temperature in the hope of the hot rerum natura of material in the temperature range in plan.
Like this, use this device, realized one-shot measurement, obtain a plurality of hot physics coefficient of material simultaneously; And can also study near room temperature material thermophysical property temperature change in net.
This error in measure:
The category-A uncertainty of measuring is with the uncertainty of theory of errors estimation end product.Under equal state, the reproduction error of duplicate measurements is better than 2.0%.
The category-B uncertainty of measuring, according to theoretical analysis: hot pin self heat absorption can not be omitted the influence of measuring, and should be revised.The influence of other factors amounts to and is not more than 0.2%, can be not significant.

Claims (5)

1. a hot rerum natura transient measurement method is placed a cylindric hot pin based in even, infinitely great medium, continues heating by hot pin to medium with constant heat flux, forms one dimension face of cylinder heat transfer model radially, and this heat transfer model is characterized by following formula:
Figure FSA00000387323800011
(1)
Figure FSA00000387323800013
Figure FSA00000387323800014
In the formula:
Figure FSA00000387323800015
In the expression detected materials, the distance of the hot pin of distance axis is the r place,
τ=t-t 0Temperature variation in time;
t 0(s) for adding the initial moment of thermal measurement;
T (r, t) (℃) for the hot pin of distance axis in the medium is the r distant place, t temperature constantly;
T (r, t 0) (℃) for the hot pin of distance axis in the medium is the r distant place, add the temperature in the initial moment of thermal measurement;
Figure FSA00000387323800016
Thermal diffusion coefficient for detected materials;
Figure FSA00000387323800017
Density for detected materials;
The quality of the certain detected materials of m (kg) expression;
V (m 3) represent the volume of this certain detected materials;
c pThe specific heat at constant pressure of J/ (kgk) expression detected materials;
The thermal conductivity of λ W/ (mk) expression detected materials;
Figure FSA00000387323800018
Represent the thermal power that hot pin unit length is sent, or claim calorific intensity;
Effective heated length of the hot pin of l (m) expression;
W=I 2The heating power of the hot pin of R (W) expression;
I (A) is by the strength of current of the heating current of hot pin;
The resistance of the hot pin heater of R (Ω);
The above-mentioned pulse cracking of separating problem surely is
Figure FSA00000387323800021
When continuing heating with constant heat flux, i.e. in the time from τ=0 to τ, r place in the test specimen, the temperature rise that the τ time is interior, an integration of available above-mentioned pulse cracking obtains; This integration can be expressed as a straight line equation approx
Figure FSA00000387323800022
In the formula: slope
Figure FSA00000387323800023
Intercept
Figure FSA00000387323800024
Here, C *=1.78115, be integration constant;
Calculate the thermal conductivity and the thermal diffusion coefficient of material:
With measuring in heat time heating time the temperature of acquisition-time logarithm ordered series of numbers T (r 0, t)~and lnt, make linear fit with young waiter in a wineshop or an inn's rule, calculate the k of the 1st sample, D then has
Thermal conductivity
Figure FSA00000387323800025
Thermal diffusion coefficient
Figure FSA00000387323800026
With corresponding medial temperature
Figure FSA00000387323800027
From i=1, choose j sample in succession; Repeat aforementioned calculation, make up database [λ j, a j, T j]; Then, do conic fitting, draw the experimental formula of calculating thermal conductivity and thermal diffusion coefficient with young waiter in a wineshop or an inn's rule
λ(T)=η 01T+η 2T 2 [T 1,T 2] (8)
a(T)=ζ 01T+ζ 2T 2 [T 1,T 2] (9)
Calculate the thermal conductivity and the thermal diffusion coefficient λ of match intermediate value temperature correspondence, a;
Bulk density and specific heat at constant pressure
Density
Figure FSA00000387323800028
Specific heat at constant pressure
Figure FSA00000387323800031
2. based on the device of the described method of claim 1, it is characterized in that: comprise dc current stabilized power supply, hot pin, temperature signal collection module, signal processor, storer, display, described hot pin is cylindric, makes with insulating material, and post contains thermocouple and electrical heating elements; Described storer prestores the computation model of thermal physical property parameter, and described dc current stabilized power supply is powered to temperature collect module; Thermocouple output temperature signal, the temperature signal collection module converts this temperature signal to digital signal, sends into signal processor, and signal processor is handled according to the computation model of thermal physical property parameter, and result is shown by display.
3. device according to claim 2, it is characterized in that: the cylinder of described hot pin is made with carbon fiber, constitute by stem stem and sleeve combination, on stem stem, this double end copper-manganese enameled wire is to form along mid point doubling coiling with a copper-manganese enameled wire to described electrical heating elements with double end copper-manganese enameled wire; Described thermocouple connects with the copper cash of thermocouple level and each root bead of constantan line and forms.
4. device according to claim 2 is characterized in that: described dc current stabilized power supply output DC stream is accurate adjustable between 0.01-1.000A; In the time of thermal measurement, the fluctuating range of heating current: Δ I≤± 0.001A.
5. device according to claim 2 is characterized in that: the temperature resolution of described temperature collect module: Δ T≤0.1k; Sample frequency: adjustable continuously between the 0.5-1Hz.
CN201010590586.3A 2010-12-10 2010-12-10 Thermal-property transient measurement method and device Expired - Fee Related CN102183544B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201010590586.3A CN102183544B (en) 2010-12-10 2010-12-10 Thermal-property transient measurement method and device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201010590586.3A CN102183544B (en) 2010-12-10 2010-12-10 Thermal-property transient measurement method and device

Publications (2)

Publication Number Publication Date
CN102183544A true CN102183544A (en) 2011-09-14
CN102183544B CN102183544B (en) 2014-01-29

Family

ID=44569765

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201010590586.3A Expired - Fee Related CN102183544B (en) 2010-12-10 2010-12-10 Thermal-property transient measurement method and device

Country Status (1)

Country Link
CN (1) CN102183544B (en)

Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102608154A (en) * 2012-02-14 2012-07-25 陈昭栋 System for measuring thermal performance transiently by using pulsing method or constant current method
CN103063701A (en) * 2012-12-26 2013-04-24 中国科学院广州能源研究所 Measurement apparatus for thermal conductivity of natural gas hydrate deposit
CN103528978A (en) * 2013-11-01 2014-01-22 哈尔滨工业大学 Method for measuring thermophysical parameters of translucent material with transient photothermal signals generated by heating pulse lasers
CN103760190A (en) * 2014-01-13 2014-04-30 中国科学院广州能源研究所 Method and device for measuring heat conduction coefficient of natural gas hydrate in porous medium
CN106199061A (en) * 2016-08-25 2016-12-07 中国农业大学 A kind of device and method measuring soil water flow velocity based on thermal pulse method
CN109490356A (en) * 2017-09-12 2019-03-19 爱斯佩克株式会社 Thermal capacitance measuring device and thermal capacitance measuring method
CN109580708A (en) * 2018-12-27 2019-04-05 西南科技大学 The voltage measurement method of the hot physical property of heat-pole method instantaneous measurement material
CN109884115A (en) * 2019-03-15 2019-06-14 东南大学 The measuring method of soil body horizontal thermal conductivity factor in situ
CN113030164A (en) * 2021-03-05 2021-06-25 湘潭大学 Metal material thermal parameter comprehensive evaluation method based on induction heating
CN116007793A (en) * 2022-11-17 2023-04-25 中国人民解放军国防科技大学 Transient thermal dose measuring device and method based on mercury thermometer

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI588485B (en) * 2015-12-02 2017-06-21 財團法人金屬工業研究發展中心 Measuring device for thermal physical parameter and needle

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101320028A (en) * 2008-05-30 2008-12-10 西安交通大学 Experiment platform for fluid thermophysical property measurement
CN101776628A (en) * 2010-01-29 2010-07-14 中国科学技术大学 Heat conductivity measuring device and method

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101320028A (en) * 2008-05-30 2008-12-10 西安交通大学 Experiment platform for fluid thermophysical property measurement
CN101776628A (en) * 2010-01-29 2010-07-14 中国科学技术大学 Heat conductivity measuring device and method

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
《中国计量学院学报》 20080630 潘江等 瞬态热线法导热系数测量的数值模拟 第108-109页 第19卷, 第2期 *
《制冷空调与电力机械》 20100630 杨文兵等 热探针法测定含湿土壤的导热系数 13-15页 第31卷, 第3期 *
《大学物理》 20070731 杨振萍等 热线法测量材料热导率 40-42页 第26卷, 第7期 *

Cited By (15)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102608154A (en) * 2012-02-14 2012-07-25 陈昭栋 System for measuring thermal performance transiently by using pulsing method or constant current method
CN103063701A (en) * 2012-12-26 2013-04-24 中国科学院广州能源研究所 Measurement apparatus for thermal conductivity of natural gas hydrate deposit
CN103528978A (en) * 2013-11-01 2014-01-22 哈尔滨工业大学 Method for measuring thermophysical parameters of translucent material with transient photothermal signals generated by heating pulse lasers
CN103528978B (en) * 2013-11-01 2016-04-20 哈尔滨工业大学 The transient state Photothermal Signals utilizing pulsed laser heating to produce measures the method for trnaslucent materials thermal physical property parameter
CN103760190A (en) * 2014-01-13 2014-04-30 中国科学院广州能源研究所 Method and device for measuring heat conduction coefficient of natural gas hydrate in porous medium
CN103760190B (en) * 2014-01-13 2016-01-27 中国科学院广州能源研究所 A kind of method and apparatus measuring gas hydrate coefficient of heat conductivity in porous medium
CN106199061A (en) * 2016-08-25 2016-12-07 中国农业大学 A kind of device and method measuring soil water flow velocity based on thermal pulse method
CN106199061B (en) * 2016-08-25 2019-07-26 中国农业大学 A kind of device and method based on thermal pulse method measurement soil water flow velocity
CN109490356A (en) * 2017-09-12 2019-03-19 爱斯佩克株式会社 Thermal capacitance measuring device and thermal capacitance measuring method
CN109490356B (en) * 2017-09-12 2021-09-28 爱斯佩克株式会社 Thermal capacity measuring apparatus and thermal capacity measuring method
CN109580708A (en) * 2018-12-27 2019-04-05 西南科技大学 The voltage measurement method of the hot physical property of heat-pole method instantaneous measurement material
CN109884115A (en) * 2019-03-15 2019-06-14 东南大学 The measuring method of soil body horizontal thermal conductivity factor in situ
CN113030164A (en) * 2021-03-05 2021-06-25 湘潭大学 Metal material thermal parameter comprehensive evaluation method based on induction heating
CN116007793A (en) * 2022-11-17 2023-04-25 中国人民解放军国防科技大学 Transient thermal dose measuring device and method based on mercury thermometer
CN116007793B (en) * 2022-11-17 2024-02-06 中国人民解放军国防科技大学 Transient thermal dose measuring device and method based on mercury thermometer

Also Published As

Publication number Publication date
CN102183544B (en) 2014-01-29

Similar Documents

Publication Publication Date Title
CN102183544B (en) Thermal-property transient measurement method and device
CN104535609B (en) A kind of heat conducting coefficient measurement device
CN104502402B (en) A kind of method for measuring the hot physical property of column heat-barrier material
CN1877313B (en) Method and apparatus for measuring solid interface contact heat exchange coefficient
CN102829888B (en) Method for eliminating three-wire heating resistor measurement errors
CN104155336B (en) Measure low-dimensional materials thermal conductivity, thermal diffusivity and the method and system of thermal capacitance simultaneously
JPS5822973B2 (en) Red bean sprouts
CN101788513A (en) Measurement device of thermal conductivity of materials and method thereof
CN208334251U (en) A kind of heat dissipation index measurement device
WO2019184076A1 (en) Method for measuring heterogeneous content of finite-thickness material based on virtual heat source principle
CN106226351B (en) A kind of thin-wall circular tube material thermal conductivity calculation method
CN201281694Y (en) Device for measuring material thermal coefficient
CN103134834A (en) Device and method for measuring dryness of wet steam
CN106124078A (en) A kind of method using double-thermocouple to measure strong transient fluid temperature
CN109557374A (en) The test device and method of small resistive element temperature-coefficient of electrical resistance
CN108318517A (en) Change the heat analysis method and device for stablizing heating based on sample parameters
CN203465028U (en) Multi-channel temperature monitor based on NTC temperature sensor
CN113008935A (en) In-situ measuring device and method for water content, thermal characteristics and electric conductivity of soil
CN115326868A (en) Device and method for measuring surface convection heat transfer coefficient of PTC heating element of fan heater
CN101762619B (en) Testing device of powder material infrared emissivity and testing method thereof
CN105973504A (en) 77K-90K temperature zone thermocouple calibration system and method
CN108051473A (en) Thermo TDR measuring method and device based on probe spacing correction
CN114047223A (en) Two sample coefficient of heat conductivity measuring device of steady state method
CN108593706A (en) A kind of both ends heating distribution transformer winding material nondestructive detection system
CN108072680A (en) A kind of use for laboratory heat conductivity of heat-conduction silicone grease evaluating apparatus

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20140129

Termination date: 20181210

CF01 Termination of patent right due to non-payment of annual fee