JP2846590B2 - Temperature compensation method for physical quantity of fluid - Google Patents

Temperature compensation method for physical quantity of fluid

Info

Publication number
JP2846590B2
JP2846590B2 JP30178594A JP30178594A JP2846590B2 JP 2846590 B2 JP2846590 B2 JP 2846590B2 JP 30178594 A JP30178594 A JP 30178594A JP 30178594 A JP30178594 A JP 30178594A JP 2846590 B2 JP2846590 B2 JP 2846590B2
Authority
JP
Japan
Prior art keywords
temperature
standard
measured
physical quantity
fluid
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
Application number
JP30178594A
Other languages
Japanese (ja)
Other versions
JPH08159944A (en
Inventor
賢治 川口
佳美 山口
喬一 松尾
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.)
KITAKYUSHU KOKA KOORA BOTORINGU KK
KYOTO DENSHI KOGYO KK
Original Assignee
KITAKYUSHU KOKA KOORA BOTORINGU KK
KYOTO DENSHI KOGYO KK
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 KITAKYUSHU KOKA KOORA BOTORINGU KK, KYOTO DENSHI KOGYO KK filed Critical KITAKYUSHU KOKA KOORA BOTORINGU KK
Priority to JP30178594A priority Critical patent/JP2846590B2/en
Publication of JPH08159944A publication Critical patent/JPH08159944A/en
Application granted granted Critical
Publication of JP2846590B2 publication Critical patent/JP2846590B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は、被検流体の物理量の温
度補償方法に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for compensating a physical quantity of a test fluid for temperature.

【0002】[0002]

【従来の技術】果汁原液や果汁飲料、清涼飲料の糖度を
表す指標として重用されているブリックス値は、例えば
密度や屈折率等を高精度に測定できる測定機器で測定
し、該測定された物理量より所定の関係に基づいて算出
される。
2. Description of the Related Art The Brix value, which is frequently used as an index indicating the sugar content of an undiluted juice, a juice beverage, and a soft drink, is measured by, for example, a measuring instrument capable of measuring density, refractive index, etc. with high accuracy, and the measured physical quantity is measured. It is calculated based on a more predetermined relationship.

【0003】この場合、ブリックス値は流体温度が20
℃であるときを以て標準温度として規定されているた
め、上記密度または屈折率とともに被検流体の温度を測
定し、例えば下記に示すような温度補償式(1) に基づい
て上記密度または屈折率の測定値に対する温度補償を行
い、温度補償後の標準値を用いてブリックス値を算出す
るようにしている。
In this case, the Brix value is determined when the fluid temperature is 20.
° C, the temperature of the test fluid is measured together with the density or the refractive index, and the density or the refractive index is measured based on the temperature compensation formula (1) shown below, for example. Temperature compensation is performed on the measured value, and the Brix value is calculated using the standard value after the temperature compensation.

【0004】 dA0=dAT×{1−αΔt−β(Δt)2 } (1) 尚、上記温度補償式(1) 中、dAT:ある被検流体Aの物
理量(密度もしくは屈折率)に関する測定値、dA0:同
じく標準温度T0 の下での標準値、Δt:温度T・標準
温度T0 (=20℃) 間の温度差であり、またα,β
は上記被検流体Aに固有の補償係数である。
D A0 = d AT × {1−αΔt−β (Δt) 2 } (1) In the above temperature compensation equation (1), d AT is a physical quantity (density or refractive index) of a certain test fluid A. D A0 : standard value under standard temperature T 0 , Δt: temperature T / standard temperature T 0 (= 20 ° C.) Temperature difference between α and β
Is a compensation coefficient specific to the test fluid A.

【0005】[0005]

【発明が解決しようとする課題】ところで、上記温度補
償式(1) の補償係数α,βは、上記被検流体Aに固有で
あるため、別の組成の被検流体に対して同様に物理量の
温度補償を実施しようとする場合には、上記補償係数
α,βとは異なる別の値の補償係数を用いる必要があっ
た。
Since the compensation coefficients α and β in the temperature compensation equation (1) are specific to the test fluid A, the physical quantities are similarly calculated for the test fluid having another composition. In order to perform the temperature compensation described above, it is necessary to use a compensation coefficient having a different value from the compensation coefficients α and β.

【0006】従って、上記温度補償を清涼飲料に対して
適用する場合、清涼飲料の種類が違えば組成も異なるた
め、清涼飲料の種類毎に多数の補償係数の組み合わせを
予め実験的に求めなければならなかった。しかも、この
ような多数の補償係数を記憶するとともに清涼飲料の種
類に応じて温度補償式に採用する補償係数を切り換える
機能を測定機器に付加しなくてはならない煩雑さがあ
る。
Therefore, when the above-mentioned temperature compensation is applied to soft drinks, different kinds of soft drinks have different compositions. Therefore, a combination of a large number of compensation coefficients must be experimentally determined in advance for each kind of soft drink. did not become. In addition, there is a problem that a function of storing such a large number of compensation coefficients and switching a compensation coefficient used in the temperature compensation equation according to the type of the soft drink must be added to the measuring instrument.

【0007】さらに、清涼飲料メーカーでは恒常的に新
製品の開発が実施されており、新製品のブリックス値の
測定を実施する前には必ず該新製品に対応する補償係数
を、多大の労力と時間を費やして実験的に決定しなけれ
ばならなかった。
[0007] Furthermore, soft drink manufacturers are constantly developing new products. Before measuring the Brix value of a new product, a compensation coefficient corresponding to the new product must be determined with a great deal of labor and labor. Spent time and had to be determined experimentally.

【0008】本発明は上記従来の事情に鑑み提案された
ものであって、ある温度の下での被検流体の物理量と該
温度とが測定されれば、該被検流体の組成を考慮するこ
と無く温度補償後の物理量を求めることができるように
した温度補償方法を提供することを目的とするものであ
る。
The present invention has been proposed in view of the above-mentioned conventional circumstances. If the physical quantity of a test fluid at a certain temperature and the temperature are measured, the composition of the test fluid is considered. It is an object of the present invention to provide a temperature compensation method capable of obtaining a physical quantity after temperature compensation without any problem.

【0009】[0009]

【課題を解決するための手段】上記の目的を達成するた
めに、本発明は以下の手段を採用する。すなわち、被検
流体の温度Tに応じて変位する該被検流体の密度もしく
は屈折率の測定値dTを、上記温度Tに基づいて標準温
度T0 における標準値d0 に補償する物理量の温度補償
方法において、上記測定値dT と、上記温度T・標準温
度T0 間の温度差Δtとを変数とする、図1に示すよう
な三次元空間内の連続曲面Dを実験的に特定し、該連続
曲面Dに基づいて上記測定値dT と温度差Δtとより標
準値d0を算出するようにした流体の物理量の温度補償
方法である。
In order to achieve the above object, the present invention employs the following means. That is, the measured value d T of the density or refractive index of the test fluid displaced in accordance with the temperature T of the test fluid is converted into the temperature of a physical quantity that compensates for the standard value d 0 at the standard temperature T 0 based on the temperature T. In the compensation method, a continuous curved surface D in a three-dimensional space as shown in FIG. 1 is experimentally specified using the measured value d T and the temperature difference Δt between the temperature T and the standard temperature T 0 as variables. A method of compensating for a physical quantity of a fluid in which a standard value d 0 is calculated from the measured value d T and the temperature difference Δt based on the continuous curved surface D.

【0010】[0010]

【作用】図1に示すように、上記三次元空間内に特定さ
れた連続曲面Dによれば、上記測定値dT と上記温度差
Δtとさえ測定されれば、両者の組み合わせと対応する
点を上記連続曲面D上に求めれば直ちに標準値d0 が算
出されることになり、該温度補償にあたっては被検流体
の組成等を斟酌する必要が全くなくなる。
As shown in FIG. 1, according to the continuous curved surface D specified in the three-dimensional space, if only the measured value d T and the temperature difference Δt are measured, a point corresponding to the combination of the two is obtained. Is obtained on the continuous curved surface D, the standard value d 0 is immediately calculated, and there is no need to take into account the composition of the test fluid in the temperature compensation.

【0011】[0011]

【実施例】図1は清涼飲料を被検流体として本発明を比
重の温度補償に適用した実施例を示す概念図である。
1 is a conceptual diagram showing an embodiment in which the present invention is applied to temperature compensation of specific gravity using a soft drink as a test fluid.

【0012】図1に示す3次元空間内の各点は、座標
(dT ,Δt,d0 )で表すことができるものとしてい
る。但し、上記において、dT :測定比重(密度)、Δ
t:比重測定時の清涼飲料の温度と標準温度20℃との
温度差、d0 :標準温度20℃への温度補償後の標準比
重である。
Each point in the three-dimensional space shown in FIG. 1 can be represented by coordinates (d T , Δt, d 0 ). However, in the above, d T : measured specific gravity (density), Δ
t: temperature difference between the temperature of the soft drink at the time of specific gravity measurement and the standard temperature of 20 ° C., d 0 : standard specific gravity after temperature compensation to the standard temperature of 20 ° C.

【0013】このような3次元空間において、既知の標
準比重dA0を有する清涼飲料Aに対して、種々の温度条
件、すなわち上記温度差Δtを設定し、各条件の下での
測定比重dATを測定し、このようにして得られた座標
(dAT,Δt,dA0)に対応する点を上記3次元空間内
に順次プロットする。このとき、上記標準値dA0は一定
であるころから、該3次元空間内にはd0 =dA0なる方
程式で表される平面上に1本の曲線が描かれることにな
る。
In such a three-dimensional space, various temperature conditions are set for the soft drink A having a known standard specific gravity d A0 , that is, the temperature difference Δt, and the measured specific gravity d AT under each condition is set. Are measured, and points corresponding to the coordinates (d AT , Δt, d A0 ) obtained in this way are sequentially plotted in the three-dimensional space. At this time, since the standard value d A0 is constant, one curve is drawn on the plane represented by the equation d 0 = d A0 in the three-dimensional space.

【0014】さらに上記清涼飲料とは異なる種類、すな
わち標準比重d0 の異なる他の清涼飲料についても同様
に種々の温度条件に対応する測定比重dT を測定し、3
次元空間内に順次プロットし、上記清涼飲料Aに対応す
る曲線とは交わることのない曲線が描かれる。もっと
も、上記複数の曲線は比重の温度係数によっては、相互
に交わることがあり得るが、少なくとも各種清涼飲料に
ついて実験的に確認した結果は、交わることはなかっ
た。
Further, for other kinds of soft drinks different from the above-mentioned soft drinks, that is, other soft drinks having different standard specific gravities d 0 , similarly, the measured specific gravity d T corresponding to various temperature conditions is measured.
Curves that are sequentially plotted in the dimensional space and do not intersect with the curve corresponding to the soft drink A are drawn. More
However, depending on the temperature coefficient of specific gravity,
, But at least in various soft drinks
The results confirmed experimentally do not intersect
Was.

【0015】このようにして、上記3次元空間内に描か
れた複数の曲線に基づいて、図1に示すような連続曲面
Dを特定することができる。上記のようにして得られた
連続曲面Dに基づけば、ある清涼飲料の測定比重と、該
測定時の清涼飲料の温度とが測定されれば、上記連続曲
面Dを特定するにあたって参考にされなかった種類の清
涼飲料においても、その標準比重を求めることができ
る。
In this manner, a continuous curved surface D as shown in FIG. 1 can be specified based on a plurality of curves drawn in the three-dimensional space. Based on the continuous curved surface D obtained as described above, if the measurement specific gravity of a certain soft drink and the temperature of the soft drink at the time of the measurement are measured, it is not referred to in specifying the continuous curved surface D. The standard specific gravity can be determined for different types of soft drinks.

【0016】すなわち、上記連続曲面Dを特定するにあ
たって参考にされなかった清涼飲料Bの標準比重dB0
求める場合には、まず該清涼飲料Bの測定比重dBTと、
該測定時の清涼飲料Bの温度と標準温度20℃との温度
差ΔtB とを測定し、図1に示すように、該当する座標
に対応する点PB を上記連続曲面D上に求め、この点P
B の座標より標準比重dB0を得ることができる。
That is, when determining the standard specific gravity d B0 of the soft drink B, which was not referred to in specifying the continuous curved surface D, first, the measured specific gravity d BT of the soft drink B was calculated as follows:
The temperature difference Δt B between the temperature of the soft drink B at the time of the measurement and the standard temperature 20 ° C. is measured, and as shown in FIG. 1, a point P B corresponding to the corresponding coordinates is obtained on the continuous curved surface D, This point P
The standard specific gravity d B0 can be obtained from the coordinates of B.

【0017】また、このようにして得られた標準比重d
B0は、該清涼飲料Bが上記標準温度20℃となるように
厳密に温度調整を行った上で測定された測定比重と測定
誤差の範囲内で一致していた。
The standard specific gravity d thus obtained is
B0 was in agreement with the measured specific gravity measured after the temperature of the soft drink B was strictly adjusted so that the standard temperature was 20 ° C. within the range of the measurement error.

【0018】このように清涼飲料一般に対して上記連続
曲面Dを適用することにより、清涼飲料の種類が変わる
度に採用する補償係数を変更したり、実験的に補償係数
を特定する作業を全く行うことなく、測定比重dT と温
度差Δtとの2つの測定値より精度の高い標準比重d0
を算出することができるようになった。これによって個
々の清涼飲料の測定作業はもとより、新製品の開発に伴
う未知の成分の清涼飲料水に対しても統一した手順でブ
リックス値を算出することができるようになった。
As described above, by applying the continuous curved surface D to a refreshing beverage in general, a compensation coefficient to be employed is changed every time the type of the refreshing beverage changes, or an operation for specifying the compensation factor experimentally is performed at all. And a standard specific gravity d 0 that is more accurate than the two measured values of the measured specific gravity d T and the temperature difference Δt.
Can be calculated. As a result, the Brix value can be calculated by a unified procedure not only for the measurement of individual soft drinks but also for soft drinks of unknown components accompanying the development of new products.

【0019】尚、本発明は上記実施例に限定されず、例
えば上記比重に代えて屈折率のような物理量に対して
も、同様の手順で連続曲面を別途特定することができる
ことは明らかであり、さらに上記温度補償が実施される
被検流体の物理量に対しても有用な方法であるといえ
る。
It should be noted that the present invention is not limited to the above-described embodiment, and it is apparent that a continuous curved surface can be separately specified in the same procedure for a physical quantity such as a refractive index instead of the above specific gravity. It can be said that this method is also useful for the physical quantity of the test fluid on which the temperature compensation is performed.

【0020】[0020]

【発明の効果】以上のように、本発明によれば、従来で
は被検流体の種類が変更される度にそれに対応する補償
係数を用いるという煩雑な作業が全く不要となり、密度
もしくは屈折率の測定値とそのときの被検流体の温度と
より一義的に標準値を特定することができる。
As described above, according to the present invention, every time the type of the test fluid is changed, the complicated operation of using the corresponding compensation coefficient is not required at all, and the density or the refractive index can be reduced. The standard value can be specified more uniquely with the measured value and the temperature of the test fluid at that time.

【0021】特に、補償係数が未知であるような新規な
被検流体に対しても全く同じ手順で標準値を算出するこ
とができるので、温度補償を実施するに伴う作業負担が
大幅に軽減される。
In particular, since a standard value can be calculated in exactly the same procedure for a new test fluid whose compensation coefficient is unknown, the work load involved in performing temperature compensation is greatly reduced. You.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明に係る一実施例の概念図である。FIG. 1 is a conceptual diagram of one embodiment according to the present invention.

【符号の説明】[Explanation of symbols]

0 標準値 dT 測定値 Δt 測定時の温度と標準温度との温度差 D 連続曲面d 0 standard value d T measured value Δt Temperature difference between measured temperature and standard temperature D Continuous curved surface

───────────────────────────────────────────────────── フロントページの続き (72)発明者 松尾 喬一 佐賀県三養基郡基山町大字長野字日渡 380番16北九州コカ・コーラボトリング 株式会社内 (58)調査した分野(Int.Cl.6,DB名) G01N 9/00 - 9/36──────────────────────────────────────────────────続 き Continuing on the front page (72) Inventor Kyoichi Matsuo 380-16 Hidari, Nagano, Kiyama-cho, Miyoki-gun, Saga Prefecture Kitakyushu Coca-Cola Bottling Co., Ltd. (58) Field surveyed (Int.Cl. 6 , DB name) ) G01N 9/00-9/36

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 被検流体の温度(T) に応じて変位する該
被検流体の密度又は屈折率の測定値(dT ) を、上記温度
(T) に基づいて標準温度(T0)における標準値(d0)に補償
する流体の物理量の温度補償方法において、 上記測定値(dT ) と上記温度(T) ・標準温度(T0)間の温
度差( Δt)と上記標準温度(T 0 )における標準値(d 0 )を変
数とする相互に交わらない範囲の複数のサンプルに対応
する複数の曲線に基づく三次元空間内の連続曲面(D) を
実験的に特定し、該連続曲面(D) に基づいて上記測定値
(dT ) と温度差( Δt)より標準値(d0)を算出するように
したことを特徴とする流体の物理量の温度補償方法。
The measured value (d T ) of the density or refractive index of the test fluid displaced in accordance with the temperature (T) of the test fluid is calculated as the temperature
Standard values at standard temperature (T 0) on the basis of the (T) at a temperature compensation method of a physical quantity of fluid to compensate (d 0), the measured value (d T) and the temperature (T) · standard temperature (T 0 ) And the standard value (d 0 ) at the standard temperature (T 0 )
Supports multiple samples that do not intersect with each other
Experimentally identify a continuous surface (D ) in a three-dimensional space based on a plurality of curved lines , and calculate the measured values based on the continuous surface (D).
A temperature compensation method for a physical quantity of a fluid, wherein a standard value (d 0 ) is calculated from (d T ) and a temperature difference (Δt).
JP30178594A 1994-12-06 1994-12-06 Temperature compensation method for physical quantity of fluid Expired - Fee Related JP2846590B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP30178594A JP2846590B2 (en) 1994-12-06 1994-12-06 Temperature compensation method for physical quantity of fluid

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP30178594A JP2846590B2 (en) 1994-12-06 1994-12-06 Temperature compensation method for physical quantity of fluid

Publications (2)

Publication Number Publication Date
JPH08159944A JPH08159944A (en) 1996-06-21
JP2846590B2 true JP2846590B2 (en) 1999-01-13

Family

ID=17901148

Family Applications (1)

Application Number Title Priority Date Filing Date
JP30178594A Expired - Fee Related JP2846590B2 (en) 1994-12-06 1994-12-06 Temperature compensation method for physical quantity of fluid

Country Status (1)

Country Link
JP (1) JP2846590B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103674772B (en) * 2013-11-27 2015-10-28 安徽秋田电子有限公司 The temperature compensation of diesel oil density

Also Published As

Publication number Publication date
JPH08159944A (en) 1996-06-21

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