CN201222042Y - Apparatus for measuring material thermal conductivity parameter - Google Patents
Apparatus for measuring material thermal conductivity parameter Download PDFInfo
- Publication number
- CN201222042Y CN201222042Y CNU2008201505662U CN200820150566U CN201222042Y CN 201222042 Y CN201222042 Y CN 201222042Y CN U2008201505662 U CNU2008201505662 U CN U2008201505662U CN 200820150566 U CN200820150566 U CN 200820150566U CN 201222042 Y CN201222042 Y CN 201222042Y
- Authority
- CN
- China
- Prior art keywords
- probe
- microprocessor system
- thermal conductivity
- probe tube
- thermopair
- 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.)
- Expired - Fee Related
Links
Images
Landscapes
- Investigating Or Analyzing Materials Using Thermal Means (AREA)
Abstract
The utility model discloses a material conductivity measuring device based on the linear heat source principle, which is characterized by comprising a probe, a microprocessor system and a stabilized voltage supply, wherein the probe comprises an electric heating cord, a probe tube and a thermocouple, the thermocouple and the heating cord are disposed in the probe tube, a probe inserted in measured material to measure the material transmits temperature potential signals to the microprocessor system, and the temperature potential signals are processed, converted and displayed by the microprocessor system, and additionally, the stabilized voltage supply provides constant voltage to the heating cord to enable the power of the heating cord to be constant, wherein the range of the voltage is controlled by the microprocessor system. The utility model increases application scope of hot-wire measurement, any object which can be plugged in a probe can be measured by the probe, repeatability and accuracy of measurement can be guaranteed after the probe is processed, further, as a computer is utilized to directly display measured results, by automatic operational program of the computer, results can be displayed on the computer only by inserting the probe into the material to-be-tested, and thereby the material conductivity measuring device has the advantages of convenient measurement and high measuring precision.
Description
Technical field
The utility model relates to a kind of material thermal conductivity measurement apparatus, particularly a kind of measurement mechanism with the probe measurement material thermal conductivity.
Background technology
Material thermal conductivity is measured and adopted a kind of heat-pole method measuring instrument at present, and mainly there is following problem in existing heat-pole method measuring instrument: (1) measurement range is narrower, can only measure single materials such as gas or liquid; (2) complicated operation, repeatable poor, accuracy can not guarantee.
Summary of the invention
The utility model is a problem narrow at existing heat-pole method measuring instrument measurement range, complicated operation, a kind of material thermal conductivity measurement apparatus with probe measurement has been proposed, by heating and the thermometric that utilizes probe, and with its data transmission to computing machine, and can demonstrate the coefficient of heat conductivity of material in real time by the program that in computing machine, configures, measurement range is wide, and data are accurate, relies on computing machine to reduce Operating Complexity.
Ultimate principle of the present utility model: when heating infinitely-great object with heater strip, line heat source can be regarded numerous points thermal source composition as, and each heat point source continues heat release with firm power.Through after a while, because heat conduction, off-line thermal source distance for the temperature rise at r place is in having the medium of normal rerum natura so:
Wherein:
In the formula:
Q: the power of line heat source unit length (w/m);
λ: coefficient of heat conductivity (w/m.K);
α: thermal diffusion coefficient (m2/s);
T, t0: time, initial time;
ρ: density (kg/m3);
Cp: specific heat (J/kg ℃)
After arrangement and distortion to following formula, when the enough little or sufficiently long words of test duration of diameter of probe, following formula can be deformed into so:
This formula is exactly the principle equation with probe measurement material thermal conductivity time institute foundation.
According to the characteristics of the heater strip of our designed device, as long as (diameter of electrical heating wire is 0.0762mm to the size of detected materials, and 0.0762mm * 25=1.905mm), promptly detected materials can be regarded infinitely-great object as so greater than 1.905mm.
Based on above-mentioned hot line source theoretical principle, the technical solution of the utility model is: a kind of material thermal conductivity measurement apparatus, be characterized in, it comprises probe, microprocessor system and stabilized voltage supply, described probe comprises electrical heating wire, probe tube and thermopair, thermopair and heater strip place the inside of probe tube, insert the probe of the temperature of measured material measurement material temperature signal is imported in the microprocessor system, by microprocessor system processing, conversion and demonstration; Stabilized voltage supply provides constant voltage to make heating power constant for the heating wire in the described probe, and the voltage range value of stabilized voltage supply is controlled by microprocessor system.
The ratio of described probe length and external diameter is greater than 25, and described heater strip adopts resistance to vary with temperature little constantan, at described constantan wire surface coating tetrafluoroethylene insulation course, injects after the described electrical heating wire doubling in the probe tube, and length is with the probe tube unanimity.Described thermopair adopts T type copper constantan insulation thermocouple, and the point for measuring temperature of thermopair is arranged in the middle aperture of probe tube, inserts the heat conductive silica gel of insulation in the middle of the probe tube.
The beneficial effects of the utility model are: the utility model has improved the measurement range of application of heat-pole method, and the material that can insert probe all can use sonde method, and no matter solid, liquid, gas all can; Repeatability and accuracy in the time of can guaranteeing to measure after the special processing of probe process; Owing to be to use computing machine directly to show measurement result, only need that probe is inserted detected materials and can pass through the automatic operation program of computer, can find out the result on computers, therefore have the characteristics convenient, that precision is high of measuring.
Description of drawings
Fig. 1 is the principle schematic of the utility model material thermal conductivity measurement apparatus;
Embodiment
Material thermal conductivity measurement apparatus comprises probe, microprocessor system and stabilized voltage supply three parts as shown in Figure 1.The main effect of probe is to insert the temperature of measured material to its heating and mensuration material; Probe comprises electrical heating wire 3, probe tube 4 and thermopair 5, thermopair 5 and electrical heating wire 3 place the inside of probe tube 4, the temperature signal that during measurement probe is recorded is imported microprocessor system 1 by the data acquisition board that is connected with microprocessor system 1 with data.The main effect of microprocessor system 1 is that whole test system is controlled, promptly the temperature measured of acquisition probe, temperature data handled, controls the voltage of stabilized voltage supply 2.The effect of stabilized voltage supply 2 is for heater strip provides constant voltage, so that heater strip is in when heating, heating power is constant.
Choosing probe length is 53mm, and external diameter is 0.7mm, and its length-diameter ratio is 75.7, makes ratio be far longer than 25, satisfies the condition (length-diameter ratio must greater than 25) of Blackwell well.Heater strip 3 adopts resistance to vary with temperature little constantan (diameter 0.0762mm), injects after heater strip 3 doublings in the probe tube 4, and length is with probe tube 4 unanimities, and heater strip 3 surfaces scribble the teflon insulation layer; Thermopair 5 adopts T type copper constantan insulation thermocouple (diameter 0.0762mm), the point for measuring temperature of thermopair 5 is arranged in the aperture of probe tube 4 centres, do not draw from aperture, insert the heat conductive silica gel of insulation in the middle of the probe tube 4, the probe tube root is fixed on the insulcrete.
Utilize the hot line ratio juris by measuring probe in difference temperature rise constantly, obtain the temperature rise slope of logarithm in time, carry it into according to heat-pole method and calculate in the middle of the formula of back institute abbreviation, just can calculate the coefficient of heat conductivity of material again according to the heating power of probe.All computation schemas set in microprocessor system, by obtain temperature-time curve in conjunction with heating power can be very fast calculate material to coefficient of heat conductivity.The characteristics of this measurement mechanism are that measurement is easy to use, and broad application temperature range can be measured frozen material, and suitable material is wide, the precision height.
Claims (4)
1, a kind of material thermal conductivity measurement apparatus, it is characterized in that, comprise probe, microprocessor system and stabilized voltage supply, described probe comprises electrical heating wire, probe tube and thermopair, thermopair and heater strip place the inside of probe tube, the probe that inserts the temperature of measured material measurement material enters the temperature electric potential signal in the microprocessor system, by microprocessor system processing, conversion and demonstration; Stabilized voltage supply provides constant voltage to make heating power constant for the heating wire in the described probe, and the voltage range value of stabilized voltage supply is controlled by microprocessor system.
According to the described material thermal conductivity measurement apparatus of claim 1, it is characterized in that 2, the ratio of described probe length and external diameter is greater than 25.
3, according to the described material thermal conductivity measurement apparatus of claim 1, it is characterized in that the described electrical heating wire that is used for probe adopts constantan wire, at described constantan wire surface coating tetrafluoroethylene insulation course, inject after the described electrical heating wire doubling in the probe tube, length is with the probe tube unanimity.
According to the described material thermal conductivity measurement apparatus of claim 1, it is characterized in that 4, described thermopair adopts T type copper constantan insulation thermocouple, the point for measuring temperature of thermopair is arranged in the middle aperture of probe tube, inserts the heat conductive silica gel of insulation in the middle of the probe tube.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CNU2008201505662U CN201222042Y (en) | 2008-07-07 | 2008-07-07 | Apparatus for measuring material thermal conductivity parameter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CNU2008201505662U CN201222042Y (en) | 2008-07-07 | 2008-07-07 | Apparatus for measuring material thermal conductivity parameter |
Publications (1)
Publication Number | Publication Date |
---|---|
CN201222042Y true CN201222042Y (en) | 2009-04-15 |
Family
ID=40575548
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CNU2008201505662U Expired - Fee Related CN201222042Y (en) | 2008-07-07 | 2008-07-07 | Apparatus for measuring material thermal conductivity parameter |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN201222042Y (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
RU2478936C1 (en) * | 2011-11-07 | 2013-04-10 | Федеральное государственное образовательное учреждение высшего профессионального образования "Казанский государственный архитектурно-строительный университет" КазГАСУ | Method of determining thermal conductivity coefficient of super-thin liquid heat-insulating coatings |
CN103293184A (en) * | 2013-05-24 | 2013-09-11 | 哈尔滨工业大学 | Experimental device for testing heat conductivity coefficient of building material based on quasi steady state and unsteady state methods |
CN104048993A (en) * | 2014-06-27 | 2014-09-17 | 吉林大学 | Portable in-situ shallow geotemperature and heat conductivity coefficient measurement device and testing method |
CN109580709A (en) * | 2018-12-27 | 2019-04-05 | 西南科技大学 | The method of the hot physical property of heat-pole method instantaneous measurement material |
-
2008
- 2008-07-07 CN CNU2008201505662U patent/CN201222042Y/en not_active Expired - Fee Related
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
RU2478936C1 (en) * | 2011-11-07 | 2013-04-10 | Федеральное государственное образовательное учреждение высшего профессионального образования "Казанский государственный архитектурно-строительный университет" КазГАСУ | Method of determining thermal conductivity coefficient of super-thin liquid heat-insulating coatings |
CN103293184A (en) * | 2013-05-24 | 2013-09-11 | 哈尔滨工业大学 | Experimental device for testing heat conductivity coefficient of building material based on quasi steady state and unsteady state methods |
CN103293184B (en) * | 2013-05-24 | 2015-03-25 | 哈尔滨工业大学 | Experimental device for testing heat conductivity coefficient of building material based on quasi steady state and unsteady state methods |
CN104048993A (en) * | 2014-06-27 | 2014-09-17 | 吉林大学 | Portable in-situ shallow geotemperature and heat conductivity coefficient measurement device and testing method |
CN109580709A (en) * | 2018-12-27 | 2019-04-05 | 西南科技大学 | The method of the hot physical property of heat-pole method instantaneous measurement material |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN101320007A (en) | Material thermal conductivity measurement apparatus by probe method | |
CN103293184B (en) | Experimental device for testing heat conductivity coefficient of building material based on quasi steady state and unsteady state methods | |
CN101788513A (en) | Measurement device of thermal conductivity of materials and method thereof | |
Zhang et al. | Simultaneous measurements of the thermal conductivity and thermal diffusivity of molten salts with a transient short-hot-wire method | |
CN102829888B (en) | Method for eliminating three-wire heating resistor measurement errors | |
CN104034749B (en) | Based on the method for testing of thermal contact resistance between the layer material of 3 ω methods | |
CN101303320A (en) | Quasi-stable state method solid body thermal conductivity measurement instrument | |
CN201222042Y (en) | Apparatus for measuring material thermal conductivity parameter | |
CN109613051B (en) | Device and method for measuring Seebeck coefficient of material by using contrast method | |
CN203465028U (en) | Multi-channel temperature monitor based on NTC temperature sensor | |
Zell et al. | Development of rapid response thermocouple probes for use in a batch ohmic heating system | |
Hu et al. | Transient hot wire measures thermophysical properties of organic foam thermal insulation materials | |
CN109781780A (en) | A kind of simple highly heat-conductive material thermal coefficient steady state test system | |
CN105445538A (en) | Novel calorimetric power meter for terahertz frequency range | |
CN201594082U (en) | Portable soil thermal resistivity measuring device | |
CN203587535U (en) | Device for measuring soil thermophysical parameters by adopting double-probe method | |
CN101329203A (en) | Apparatus for measuring temperature of alternating current-direct current lightning arrestor | |
CN200996949Y (en) | Steel wire thermal-expansion coefficient determiner | |
CN103630569A (en) | Method for measuring heterogeneous medium content of material based on volume thermal mass | |
CN103487174A (en) | Electric energy calibration device of gas calorimeter | |
CN204374119U (en) | Solid dynamic heat transfer coefficient measuring device and measuring system | |
CN208505485U (en) | A kind of surface temperature measurement instrument | |
CN102636524A (en) | Device for electrically transiently measuring thermo-physical properties of materials and method | |
CN202421102U (en) | Device for measuring thermal conductivity coefficient of gas | |
CN201666888U (en) | Measuring device for conductivity of material |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C14 | Grant of patent or utility model | ||
GR01 | Patent grant | ||
C17 | Cessation of patent right | ||
CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20090415 Termination date: 20110707 |