Self-calibrated flow meter

Patent metadata

Field	Value
Publication number	US-9835506-B2
Application number	US-201214366888-A
Country	US
Kind code	B2
Filing date	Dec 20, 2012
Priority date	Dec 21, 2011
Publication date	Dec 5, 2017
Grant date	Dec 5, 2017

Abstract

The present invention relates to a method for estimating the thermophysical properties of a material (Ω) that incorporates at least one temperature sensor ( 1, 2, 3 ) and one point heat source ( 4 ), the distance between the at least one temperature sensor ( 1, 2, 3 ) and the point heat source ( 4 ) being known. The method includes the steps of: expression of the theoretical temperature as a function of time at the at least one temperature sensor ( 1, 2, 3 ) when the point heat source ( 4 ) is activated, said expression depending on the thermophysical parameters of the material (Ω); acquisition of a plurality of temperature measurements by the at least one temperature sensor ( 1, 2, 3 ) over a time period during which the point heat source ( 4 ) is activated; and determining of the values of the thermophysical parameters of the material (Ω), such that the difference between the theoretical temperatures obtained via said expression and the temperatures that are actually measured is minimal. The present invention also relates to a method for measuring a heat flow (φ(t)) across a surface (Γ) of a material (Ω) and a flow meter ( 10 ) designed for this purpose.

First claim

The invention claimed is:

1. A process for estimation of the thermophysical properties of material (Ω), at least one temperature sensor and one point heat source being integrated into said material (Ω), the distance between the at least one temperature sensor and the point heat source being known, the process comprising steps of:
expression of the theoretical temperature as a function of time at the level of the at least one temperature sensor when the point heat source is activated, said expression dependent on the thermophysical parameters of the material (Ω);
acquisition of a plurality of temperature measurements by the at least one temperature sensor during a time interval during which the point heat source is activated;
determination of the values of the thermophysical parameters of the material (Ω) such that the deviation between the theoretical temperatures obtained via said expression and the temperatures effectively measured is minimal;
wherein said thermophysical properties of the material (Ω) comprise the thermal conductivity k of the material (Ω);
wherein the deviation between the F theoretical temperatures obtained {η(d,t i ,β 1 ,β 2 )} iε[1,F] and the effectively measured F temperatures {Y(d,t i )} iε[1,F] to be minimised is expressed by the formula

J
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1

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β
2

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1

F

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Y
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(

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-

η
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2

,

d being said distance between the at least one temperature sensor and the point heat source, β 1 being a parameter inversely proportional to the thermal conductivity k, and β 2 being a parameter proportional to the thermal diffusivity a.

2. A measurement process of heat flow (φ(t)) passing through a surface (Γ) of a material (Ω), at least one temperature sensor and one point heat source being integrated into said material, the distance between the at least one temperature sensor and the point heat source and the distance between the at least one temperature sensor and the surface (Γ) of the material (Ω) passed through by the heat flow (φ(t)) being known, the process comprising steps of:
measurement over time of a plurality of internal temperatures of the material (Ω) by the at least one temperature sensor;
estimation of the thermal conductivity k and of the thermal diffusivity a of the material (Ω) by the execution of the process for estimation of the thermophysical properties of a material (Ω), according to claim 1 ;
determination of the heat flow (φ(t)) passing through the surface (Γ) of the material (Ω) from the internal temperatures measured as a function of time by the at least one temperature sensor, of the estimated thermal conductivity k and the thermal diffusivity a of the material (Ω).

3. The process according to claim 2 , at least two internal temperatures are measured over time by at least two temperature sensors, one being substantially further away from the surface (Γ) of the material (Ω) passed through by the heat flow (φ(t)) than the other, the process also comprising a verification step of the condition on the limits from the internal temperature measured as a function of time by the temperature sensor further away from the surface (Γ) of the material (Ω).

4. A flow meter for measurement of heat flow (φ(t)) passing through a surface (Γ) of a material (Ω) wherein it comprises:
at least one temperature sensor integrated into a sample of the material (Ω);
a controllable point heat source, also integrated into the sample of the material (Ω);
means of acquisition of a plurality of temperature measurements by the at least one temperature sensor during a time interval;
processing means of the plurality of acquired temperature measurements capable of executing the process for measurement of heat flow (φ(t)) passing through the surface (Γ) of said material (Ω), according to claim 2 .

5. The flow meter according to claim 4 , comprising a first temperature sensor and a second temperature sensor, the first temperature sensor being closer to the surface (Γ) of the material (Ω) passed through by the heat flow (φ(t)) than the second temperature sensor, the first temperature sensor being at a known distance from the surface (Γ) of the material (Ω) passed through by the heat flow (φ(t)), the second temperature sensor being at a known distance from the point heat source, the measurements of the first sensor being used for estimation of the heat flow (φ(t)), and the measurements of the second sensor being used for estimation of the thermophysical properties of the material (Ω).

6. The flow meter according to claim 5 , comprising a third temperature sensor, of position relative to the known surface, the third temperature sensor being substantially further away from the surface (Γ) of the material (Ω) passed through by the heat flow (φ(t)) than the first and second sensors, the measurements of the third sensor being used to understand a condition on the limits of the material (Ω).

7. The flow meter according to claim 6 , wherein the third temperature sensor is at a known distance from the point heat source, in particular the same as the second temperature sensor, measurements of the third sensor being compared to measurements of the second sensor to control the homogeneity of the material (Γ).

8. The flow meter according to claim 5 , wherein the measurements of the second sensor are also used for estimation of the heat flow (φ(t)) when the point source is deactivated.

9. The flow met

Assignees

• Inst De Radioprotection Et De Sûreté Nucléaire
• Univ Aix Marseille

Inventors

• Pons Serge
• Coutin Mickaël
• Luciani Sébastien
• Le Niliot Christophe
• Rigollet Fabrice

Classifications

• G01K19/00

  Testing or calibrating calorimeters · CPC title

• G01N25/18

  by investigating thermal conductivity (by calorimetry G01N25/20; by measuring change of resistance of an electrically-heated body G01N27/18) · CPC title

• G01K17/00 Primary

  Measuring quantity of heat (measuring temperature by calorimetry G01K3/00 - G01K11/00; specially adapted for measuring thermal properties of materials, e.g. specific heat, heat of combustion G01N) · CPC title