Determining the heat flow emanating from a heat transporting fluid

US9429484B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-9429484-B2
Application numberUS-201113881275-A
CountryUS
Kind codeB2
Filing dateOct 19, 2011
Priority dateNov 18, 2010
Publication dateAug 30, 2016
Grant dateAug 30, 2016

How to read this patent

A practical reading order for non-experts. Skip the full description unless you need deep technical detail.

  1. Title

    What the patent document calls the invention.

  2. Abstract

    A short plain-language summary of the technical disclosure.

  3. Assignees and inventors

    Who owns or filed the patent and who is credited as inventor.

  4. Key dates

    Filing, priority, publication, and grant dates set the timeline.

  5. First independent claim

    The legal scope of protection — read this for what is actually claimed.

  6. CPC / IPC classifications

    Technology tags used to group this patent with similar filings.

  7. Citations and related patents

    Prior art links and similar publications in this corpus.

Abstract

Official abstract text for this publication.

The invention relates to a method for determining the heat flow (dQ/dt) emanating from a heat transporting fluid ( 12 ), which is a mixture of at least two different fluids, and which flows through a flow space ( 11 ) from a first position, where it has a first temperature (T 1 ), to a second position, where it has, due to that heat flow (dQ/dt), a second temperature (T 2 ), which is lower than said first temperature (T 1 ), whereby the density and specific heat of said heat transporting fluid ( 12 ) is determined by measuring the speed of sound (vs) in said fluid, and said density and specific heat of said heat transporting fluid ( 12 ) is used to determine the heat flow (dQ/dt).

First claim

Opening claim text (preview).

The invention claimed is: 1. A method for determining heat flow (dQ/dt) emanating from a heat transporting fluid ( 12 ), which is a mixture of at least two different fluids, and which flows through a flow space ( 11 ) from a first position, where said heat transporting fluid ( 12 ) has a first temperature (T 1 ), to a second position, where said heat transporting fluid ( 12 ) has, due to said heat flow (dQ/dt), a second temperature (T 2 ), which is lower than said first temperature (T 1 ), said method comprising the steps of: a) measuring a differential temperature (ΔT) between said first temperature (T 1 ) and said second temperature (T 2 ); b) measuring a speed of sound (v s ) within said heat transporting fluid ( 12 ) at a predetermined location of said flow space ( 11 ) in a vicinity of said first and/or second position; c) measuring an absolute temperature (T) of the heat transporting fluid ( 12 ) at said predetermined location; d) measuring a volume flow (dV/dt) at said predetermined location; e) determining from said measured absolute temperature (T) and said measured speed of sound (v s ) a mixing ratio of said heat transporting fluid ( 12 ); f) determining from said measured absolute temperature (T) and said determined mixing ratio of said heat transporting fluid ( 12 ) a density and a specific heat of said heat transporting fluid ( 12 ); and g) determining from said measured differential temperature (ΔT), said measured volume flow (dV/dt), said determined density and said determined specific heat the heat flow (dQ/dt) emanating from said heat transporting fluid ( 12 ). 2. The method according to claim 1 , characterised in that said heat transporting fluid ( 12 ) is a binary mixture of two fluids. 3. The method according to claim 2 , characterised in that said heat transporting fluid ( 12 ) is a mixture of water and an antifreeze fluid. 4. The method according to claim 3 , characterised in that said heat transporting fluid ( 12 ) is a water and glycol mixture. 5. The method according to claim 1 , characterised in that the mixing ratio of said heat transporting fluid ( 12 ) is determined from said measured absolute temperature (T) and said measured speed of sound (v s ) by means of a data table ( 21 ) for the relation between speed of sound (v s ), absolute temperature (T) and mixing ratio of the specific heat transporting fluid ( 12 ). 6. The method according to claim 1 , characterised in that the mixing ratio of said heat transporting fluid ( 12 ) is determined from said measured absolute temperature (T) and said measured speed of sound (v s ) by means of a mathematical relation between speed of sound (v s ), absolute temperature (T) and mixing ratio of the specific heat transporting fluid ( 12 ). 7. The method according to claim 1 , characterised in that the speed of sound (v s ) within said heat transporting fluid ( 12 ) is measured by means of an ultrasonic measuring arrangement ( 13 ). 8. The method according to claim 7 , characterised in that the ultrasonic measuring arrangement ( 13 ) comprises a first ultrasonic transducer ( 14 ) placed at a first side of said flow space ( 11 ) and a second ultrasonic transducer ( 15 ) is placed at a second side of said flow space ( 11 ), such that an ultrasonic signal travelling between said first and second ultrasonic transducers ( 14 , 15 ) passes the fluid ( 12 ) within said flow space ( 11 ). 9. The method according to claim 8 , characterised in that, the first and second ultrasonic transducers ( 14 , 15 ) are arranged with respect to the fluid flow within said flow space ( 11 ), such that an ultrasonic signal travelling between said first and second ultrasonic transducers ( 14 , 15 ) has a velocity component in the direction of said fluid flow, the speed of sound (v s ) is measured in opposite directions between said first and second ultrasonic transducers ( 14 , 15 ), and the volume flow (dV/dt) is derived from the measured different speeds of sound (v s ) in said opposite directions. 10. The method according to claim 8 , characterised in that the measurement of the speed of sound (v s ) is based on measuring transit time of an ultrasonic pulse travelling between said first and second ultrasonic transducers ( 14 , 15 ). 11. The method according to claim 10 , characterised in that the measurement of the speed of sound (v s ) is done according to a sing-around method. 12. The method according to claim 1 , characterised in that said volume flow (dV/dt) is measured by means of a separate flow meter ( 24 ). 13. A heat flow measuring arrangement ( 10 ) for carrying out the method according to claim 1 , said heat flow measuring arrangement ( 10 ) comprising: a) first means ( 16 , 18 ) for measuring the differential temperature (ΔT) between said first temperature (T 1 ) and said second temperature (T 2 ); b) second means ( 13 , 19 ) for measuring the speed of sound (v s ) within said heat transporting fluid ( 12 ) at a predetermined location of said flow space ( 11 ) in the vicinity of said first and/or second position; c) third means ( 17 ) for measuring the absolute temperature (T) of the heat transporting fluid ( 12 ) at said predetermined location; d) fourth means ( 13 , 24 ) for measuring the volume flow (dV/dt) at said predetermined location; whereby said first, second, third and fourth means ( 13 , 16 , 17 , 18 , 19 , 24 ) are connected to an evaluation unit ( 20 ) for determining said heat flow (dQ/dt) based on the data it receives from said first, second, third and fourth means ( 13 , 16 , 17 , 18 , 19 , 24 ). 14. The heat flow measuring arrangement according to claim 13 , characterised in that said first means for measuring the differential temperature (ΔT) comprises a first temperature probe ( 16 ) placed at said first position, and a second temperature probe ( 18 ) placed at said second position downstream of said first position. 15. The heat flow measuring arrangement according to claim 14 , characterised in that said second means for measuring the speed of sound (v s ) within said heat transporting fluid ( 12 ) at a predetermined location of said flow space ( 11 ) comprises an ultrasonic measuring arrangement ( 13 ), which is connected to an ultrasonic control unit ( 19 ). 16. The heat flow measuring arrangement according to claim 15 , characterised in that said third means for measuring the absolute temperature (T) of the heat transporting fluid ( 12 ) at said predetermined location comprises a third temperature probe ( 17 ), which is placed between said first and second temperature probes ( 16 , 18 ) in the flow direction. 17. The heat flow measuring arrangement according to claim 15 , characterised in that said fourth means for measuring the volume flow (dV/dt) at said predetermined location comprises a separate flow meter ( 24 ). 18. The heat flow measuring arrangement according to claim 15 , characterised in that said ultrasonic measuring arrangement ( 13 ) comprises at least two ultrasonic transducers ( 14 , 15 ), which are arranged, such that an ultrasonic signal travelling between said at least two ultrasonic transducers ( 14 , 15 ) passes through said heat transporting fluid ( 12 ). 19. The heat flow measuring arrangement according to claim 18 , characterised in that said at least two ultrasonic transducers ( 14 , 15 ) are arranged with respect to the flow direction of said heat transporting fluid ( 12 ), such that a measuring track between said at least two ultrasonic transducers ( 14 , 15 ) intersects said flow direction under an oblique angl

Assignees

Inventors

Classifications

  • based upon measurement of temperature difference {or of a temperature} · CPC title

  • G01K17/10Primary

    between an inlet and an outlet point, combined with measurement of rate of flow of the medium {if such, by integration during a certain time-interval} · CPC title

  • by measuring propagation velocity or propagation time of acoustic waves · CPC title

Patent family

Related publications grouped by family.

External sources

Frequently asked questions

Answers are generated from the same data shown on this page.

What does patent US9429484B2 cover?
The invention relates to a method for determining the heat flow (dQ/dt) emanating from a heat transporting fluid ( 12 ), which is a mixture of at least two different fluids, and which flows through a flow space ( 11 ) from a first position, where it has a first temperature (T 1 ), to a second position, where it has, due to that heat flow (dQ/dt), a second temperature (T 2 ), which is lower than…
Who is the assignee on this patent?
Lindgren Mats, Carlander Carl, Holoch Philip, and 1 more
What technology area does this patent fall under?
Primary CPC classification G01K17/10. Mapped technology areas include Physics.
When was this patent published?
Publication date Tue Aug 30 2016 00:00:00 GMT+0000 (Coordinated Universal Time) (B2). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 8 related publications on this page (citations in our corpus or others sharing the same primary CPC).