JPH0338535B2 - - Google Patents

Info

Publication number
JPH0338535B2
JPH0338535B2 JP17690384A JP17690384A JPH0338535B2 JP H0338535 B2 JPH0338535 B2 JP H0338535B2 JP 17690384 A JP17690384 A JP 17690384A JP 17690384 A JP17690384 A JP 17690384A JP H0338535 B2 JPH0338535 B2 JP H0338535B2
Authority
JP
Japan
Prior art keywords
value
calibration
temperature
detector
resistance
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
Application number
JP17690384A
Other languages
Japanese (ja)
Other versions
JPS6071925A (en
Inventor
Ierugensen Iuaa
Aagaaruto Kieruto
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.)
Danfoss AS
Original Assignee
Danfoss AS
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 Danfoss AS filed Critical Danfoss AS
Publication of JPS6071925A publication Critical patent/JPS6071925A/en
Publication of JPH0338535B2 publication Critical patent/JPH0338535B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01KMEASURING TEMPERATURE; MEASURING QUANTITY OF HEAT; THERMALLY-SENSITIVE ELEMENTS NOT OTHERWISE PROVIDED FOR
    • G01K7/00Measuring temperature based on the use of electric or magnetic elements directly sensitive to heat ; Power supply therefor, e.g. using thermoelectric elements
    • G01K7/16Measuring temperature based on the use of electric or magnetic elements directly sensitive to heat ; Power supply therefor, e.g. using thermoelectric elements using resistive elements
    • G01K7/18Measuring temperature based on the use of electric or magnetic elements directly sensitive to heat ; Power supply therefor, e.g. using thermoelectric elements using resistive elements the element being a linear resistance, e.g. platinum resistance thermometer
    • G01K7/20Measuring temperature based on the use of electric or magnetic elements directly sensitive to heat ; Power supply therefor, e.g. using thermoelectric elements using resistive elements the element being a linear resistance, e.g. platinum resistance thermometer in a specially-adapted circuit, e.g. bridge circuit
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01KMEASURING TEMPERATURE; MEASURING QUANTITY OF HEAT; THERMALLY-SENSITIVE ELEMENTS NOT OTHERWISE PROVIDED FOR
    • G01K17/00Measuring quantity of heat
    • G01K17/06Measuring quantity of heat conveyed by flowing media, e.g. in heating systems e.g. the quantity of heat in a transporting medium, delivered to or consumed in an expenditure device
    • G01K17/08Measuring quantity of heat conveyed by flowing media, e.g. in heating systems e.g. the quantity of heat in a transporting medium, delivered to or consumed in an expenditure device based upon measurement of temperature difference or of a temperature
    • G01K17/10Measuring quantity of heat conveyed by flowing media, e.g. in heating systems e.g. the quantity of heat in a transporting medium, delivered to or consumed in an expenditure device based upon measurement of temperature difference or of a temperature 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

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Combustion & Propulsion (AREA)
  • Measuring Temperature Or Quantity Of Heat (AREA)
  • Measuring Volume Flow (AREA)
  • Measuring And Recording Apparatus For Diagnosis (AREA)
  • Details Of Flowmeters (AREA)

Description

【発明の詳細な説明】 発明の関連する技術分野 本発明は、少なくとも1つの温度に依存する検
出器抵抗と、検出器抵抗の温度に依存する電圧降
下を処理する評価回路とを用いて温度値を測定す
る装置に関する。
DETAILED DESCRIPTION OF THE INVENTION Related Field of the Invention The present invention uses at least one temperature-dependent detector resistor and an evaluation circuit to process the temperature-dependent voltage drop across the detector resistor to determine the temperature value. This invention relates to a device for measuring.

従来技術 この形式の公知の装置では暖房装置の供給流温
度と戻り流温度とが各々1つの温度に依存する抵
抗を用いて測定される。温度測定信号変換器が温
度と共に直線的に変化する電流信号を発生する。
この電流信号は負荷抵抗を介して伝達され、この
負荷抵抗から温度に比例する電圧降下が検出され
る。さらに流量用の電流信号が供給されるので、
第3の負荷抵抗において流量に比例する電圧降下
を検出することができる。これらの電圧降下は順
次マルチプレクサを介して評価回路に供給され、
そこでA−D変換された後に中間記憶される。記
憶されたデータ表から温度に依存して取出し可能
な温度係数を用いて、温度係数と流量と乗算する
ことによつて温度差を形成して、伝達された熱量
を積分により算出し且つ指示し且つ記憶しておく
ことができる。
PRIOR ART In known devices of this type, the supply stream temperature and the return stream temperature of the heating device are each measured using a temperature-dependent resistance. A temperature measurement signal converter generates a current signal that varies linearly with temperature.
This current signal is transmitted through a load resistor from which a voltage drop proportional to temperature is detected. In addition, a current signal for flow rate is supplied, so
A voltage drop proportional to the flow rate can be detected at the third load resistance. These voltage drops are sequentially fed to the evaluation circuit via a multiplexer,
There, the data is subjected to A-D conversion and then intermediately stored. Using a temperature coefficient that can be retrieved depending on the temperature from a stored data table, the temperature difference is formed by multiplying the temperature coefficient by the flow rate, and the amount of heat transferred is calculated and indicated by integration. And it can be stored.

発明が解決しようとする問題点 検出器温度に比例する電流信号を送出すべき温
度測定信号変換器は極めてコストがかかる。また
調整も複雑である。なぜならこの形式の2つの測
定信号変換器では各々3つのポテンシオメータを
調整しなければならないからである。温度差の測
定結果には両温度測定信号変換器の許容偏差と負
荷抵抗の許容偏差とが含まれるので、小さな温度
差での測定結果に著しい誤差が生ずることがあ
る。
Problems to be Solved by the Invention Temperature measurement signal converters, which are to deliver a current signal proportional to the detector temperature, are extremely expensive. Adjustment is also complicated. This is because two measuring signal converters of this type each require three potentiometers to be adjusted. Since the measurement result of the temperature difference includes the tolerance of both temperature measurement signal converters and the tolerance of the load resistance, a significant error may occur in the measurement result with a small temperature difference.

本発明の課題は、従来に比べて所望の温度を遥
かに僅かなコストで検出でき且つ調整が遥かに容
易な、冒頭に述べた形式の温度測定装置を提供す
ることにある。
The object of the invention is to provide a temperature measuring device of the type mentioned at the outset, which can detect a desired temperature at a much lower cost and is much easier to adjust than before.

問題点を解決するための手段 この課題は本発明によれば次のような構成によ
り解決される。即ち少なくとも1つの検出器抵抗
が2つの固定較正抵抗、即ち基準抵抗および差動
抵抗との直列接続にて共通の電流源に接続されて
おり、基準抵抗は、所定の低い温度のときに検出
器抵抗が示す最小較正値を有しており、また差抵
抗の差較正値は検出器抵抗が所定の高い温度のと
きに示す最大較正値を較正抵抗の直列接続が有す
るような大きさになつており、較正値記憶装置が
設けられており、較正抵抗のうちの少なくとも1
つないし複数の較正抵抗の直列接続において少な
くとも1つの較正電圧降下を検出可能であり、ま
た各検出器抵抗において1つの測定電圧降下を検
出可能であり、評価回路が実際温度値を少なくと
も1つの測定電圧降下から、少なくとも1つの目
盛値とこれに対応する較正電圧降下とから形成さ
れる較正曲線に基づいて検出する冒頭に述べた形
式の温度測定装置。
Means for Solving the Problem This problem is solved by the following configuration according to the present invention. That is, at least one detector resistor is connected to a common current source in series with two fixed calibration resistors, namely a reference resistor and a differential resistor, the reference resistor being connected to a common current source at a predetermined low temperature. The resistor has a minimum calibrated value, and the differential calibrated value of the differential resistance is such that the series connection of the calibrated resistors has a maximum calibrated value that the detector resistance exhibits at a given high temperature. and a calibration value storage device is provided for at least one of the calibration resistors.
At least one calibrated voltage drop can be detected in the series connection of several calibration resistors and one measured voltage drop can be detected in each detector resistor, and the evaluation circuit can detect the actual temperature value in at least one measured value. A temperature measuring device of the type mentioned at the outset, which detects the voltage drop on the basis of a calibration curve formed from at least one scale value and a corresponding calibration voltage drop.

実施例 次に本発明の実施例を図面を用いて詳細に説明
する。
Embodiments Next, embodiments of the present invention will be described in detail with reference to the drawings.

第1図によれば、温度に依存する実抵抗値Rf1
を有する供給流用検出器抵抗F1と、温度に依存
する実抵抗値Rf2を有する戻り流用検出器抵抗F
2とが2つの較正抵抗、即ち基準抵抗Gと差抵抗
Dとの直列接続にて共通の電流源1に接続されて
いる。直列接続回路を流れる電流Iは例えば1m
A±5%の値を有する。基準抵抗Gは所定の値、
即ち最小較正値Re1、例えば100Ω士0.01%を有す
る。差抵抗Dも所定の値、即ち差較正値Rd、例
えば50Ω±0.01%を有する。従つて較正抵抗の直
列接続G、Dは所定の抵抗値、即ち最大較正値
Re2(この場合150Ωとなる)を有する。検出器抵
抗F1およびF2はこの実施例の場合PT100抵抗
であり、従つて最小較正値Re1は検出器抵抗の0
℃のときの抵抗値に相当し、最大較正値Re2
130℃のときの検出器抵抗の抵抗値に相当する。
電流Iが流れると、検出器抵抗F1およびF2に
おいて、測定電圧降下Vf1ないしVf2が検出され
る。較正抵抗GないしD、ないし較正抵抗の直列
回路において較正電圧降下Ve1ないしVdないし
Ve2が取出される。しかし動作中はこれらの較正
電圧降下のうちのせいぜい2つを検出しさえすれ
ばよい。残りの1つの較正電圧降下はこれらの2
つから算出することができる。
According to Figure 1, the temperature-dependent actual resistance R f1
a detector resistance F1 for the supply flow having a temperature-dependent real resistance R f2 and a detector resistance F1 for the return flow having a temperature-dependent actual resistance value R f2
2 are connected to a common current source 1 through a series connection of two calibration resistors, namely a reference resistor G and a differential resistor D. The current I flowing through the series connection circuit is, for example, 1 m.
It has a value of A±5%. The reference resistance G is a predetermined value,
That is, it has a minimum calibration value R e1 , for example 0.01% across 100Ω. The differential resistance D also has a predetermined value, ie a differential calibration value R d , for example 50Ω±0.01%. Therefore, the series connection G and D of calibration resistors has a predetermined resistance value, that is, the maximum calibration value.
It has R e2 (150Ω in this case). Detector resistances F1 and F2 are PT100 resistors in this example, so the minimum calibration value R e1 is 0 for the detector resistance.
It corresponds to the resistance value at °C, and the maximum calibration value R e2 is
Corresponds to the resistance value of the detector resistance at 130℃.
When a current I flows, a measured voltage drop V f1 or V f2 is detected across the detector resistors F1 and F2. Calibration voltage drop V e1 or V d in a series circuit of calibration resistors G or D or calibration resistors
V e2 is taken out. However, during operation, it is only necessary to detect at most two of these calibrated voltage drops. The remaining calibration voltage drop is these two
It can be calculated from one.

第2図に示すように、マルチプレクサ3の入力
側2に既述の較正電圧降下Ve1およびVe2と測定
電圧降下Vf1およびVf2、ならびに熱交換器を貫流
する際に生じる貫流電圧降下Vqとその較正に使
用される較正電圧降下Ve3とが加えられる。入力
側2は制御入力側4を介して供給されるアドレス
信号により順次呼出され、その際例えば測定電圧
降下Vf1,Vf2と貫流電圧降下Vqとが少なくとも
1秒に1度マルチプレクサ3の出力側5から取出
され、他の較正電圧降下Ve1,Ve2,Ve3は約10秒
ごとにマルチプレクサ3の出力側5から取出され
る。この出力側5は、場合によつては1つの図示
していない増幅器を介して、アナログ−デイジタ
ル変換器6(最も簡単な場合電圧制御発振器)に
接続されており、このA−D変換器はデイジタル
信号をホトカプラ7を介してマイクロプロセツサ
9の計算機回路8に送出する。マイクロプロセツ
サもマルチプレクサ3に対するアドレス信号を発
生し、このアドレス信号はマルチプレクサ3の制
御入力側4に別のホトカプラ10を介して送出さ
れる。マイクロプロセツサ9は種々異なる記憶場
所、例えばマルチプレクサ3を介して供給される
デイジタル化された信号の中間記憶のための中間
記憶装置11や、幾つかのまたはすべての較正値
Re1,Re2ないしRdが入力される入力側13を有
する記憶装置12などを有する。ホトカプラ7お
よび10により、上記のような構造を有する評価
回路の入力段14が、他の機器から電気的に分離
されている。マイクロプロセツサ9はさらに時間
基準発生器15を有し、時間基準発生器には例え
ば極めて精密に動作する水晶が設けられている。
As shown in FIG. 2, the already mentioned calibrated voltage drops V e1 and V e2 and the measured voltage drops V f1 and V f2 are present on the input side 2 of the multiplexer 3, as well as the flow-through voltage drop V that occurs when the flow passes through the heat exchanger. q and the calibration voltage drop V e3 used for its calibration are added. The inputs 2 are sequentially addressed by address signals supplied via the control inputs 4, in which case, for example, the measured voltage drops V f1 , V f2 and the flow-through voltage drop V q are activated at least once every second at the output of the multiplexer 3. Other calibration voltage drops V e1 , V e2 , V e3 are taken from the output side 5 of the multiplexer 3 approximately every 10 seconds. This output 5 is connected, possibly via an amplifier not shown, to an analog-to-digital converter 6 (in the simplest case a voltage-controlled oscillator), which The digital signal is sent to the computer circuit 8 of the microprocessor 9 via the photocoupler 7. The microprocessor also generates an address signal for the multiplexer 3, which address signal is sent via a further optocoupler 10 to the control input 4 of the multiplexer 3. The microprocessor 9 has various storage locations, for example an intermediate storage 11 for intermediate storage of the digitized signals supplied via the multiplexer 3 and some or all calibration values.
It includes a storage device 12 having an input side 13 into which R e1 , R e2 to R d are input. By means of the photocouplers 7 and 10, the input stage 14 of the evaluation circuit having the structure described above is electrically isolated from other equipment. The microprocessor 9 furthermore has a time reference generator 15, which is provided, for example, with a very precisely operated crystal.

マイクロプロセツサ9の出力側16には機器が
接続されており、この機器は2つの機械的カウン
タ17および18ならびに指示装置19を備えて
いる。カウンタ17は例えば連続的に流量を加算
し、カウンタ18は熱量を加算する。指示装置1
9は切換スイツチ20で種々異なる値に切換えら
れる。例えばこれらの値には、供給流の温度、戻
り流の温度、温度差、最低温度差、流量、流量の
目盛限界値、熱量等がある。
A device is connected to the output 16 of the microprocessor 9, which device comprises two mechanical counters 17 and 18 and an indicating device 19. For example, the counter 17 continuously adds up the flow rate, and the counter 18 adds up the amount of heat. Instructing device 1
9 can be switched to various different values by a changeover switch 20. For example, these values include supply stream temperature, return stream temperature, temperature difference, minimum temperature difference, flow rate, scale limit value of flow rate, amount of heat, etc.

別の出力側21はデイジタル−アナログ変換器
22に接続されており、このD−A変換器の出力
側23からはプログラマブル電流信号が送出さ
れ、この信号は例えば熱量、流量、供給流温度、
戻り流温度、または温度差に関している。出力電
流は例えば4〜20mAの一定の電流信号により形
成できる。
A further output 21 is connected to a digital-to-analog converter 22, the output 23 of which provides a programmable current signal, which can e.g.
It concerns the return flow temperature, or temperature difference. The output current can be generated by a constant current signal of, for example, 4 to 20 mA.

マイクロプロセツサ9のさらに別の出力側24
は複数のホトカプラ25,26,27,28に接
続されている。ホトカプラ25はカウンタ17に
同期したパルス、即ち貫流流量に同期したパルス
を発生し、ホトカプラ26はカウンタ18に同期
した、即ち熱量に同期したパルスを発生する。ホ
トカプラ27は例えば温度差が設定された最小温
度差よりも小さいときにアラーム信号を送出す
る。ホトカプラ28は例えば検出器の故障や電流
断等に依存してエラー信号を発生する。
A further output 24 of the microprocessor 9
are connected to a plurality of photocouplers 25, 26, 27, and 28. The photocoupler 25 generates pulses synchronized with the counter 17, that is, pulses synchronized with the flow rate, and the photocoupler 26 generates pulses synchronized with the counter 18, that is, pulses synchronized with the amount of heat. The photocoupler 27 sends out an alarm signal, for example, when the temperature difference is smaller than a set minimum temperature difference. The photocoupler 28 generates an error signal depending on, for example, a detector failure or a current interruption.

複数の設定スイツチ29は、熱量測定装置を
種々異なる用途に合わせて設定するのに用いられ
る。こうして例えば最小温度差またはD−A変換
器22における出力電流またはカウンタ17およ
び18に対する乗算係数を設定することができ
る。4つの切換スイツチ30では、2進化10進数
に対して0〜9999m3/hの貫流流量目盛の限界領
域を設定することができる。
A plurality of setting switches 29 are used to set the calorimeter for different applications. In this way, for example, the minimum temperature difference or the output current in the D/A converter 22 or the multiplication factor for the counters 17 and 18 can be set. With the four changeover switches 30, it is possible to set the limit range of the flow rate scale from 0 to 9999 m 3 /h in binary coded decimal notation.

第3図は電圧降下Vに関する較正抵抗値Rの経
過を示す。図示の特性曲線Kは、較正値対Re1
Ve1とRe2/Ve2とRd/Vdのうちの2つを使用す
るとき、これらの使用したデータに基き如何に表
わされるかを示す。さらに、測定電圧効果下Vf1
ないしVf2が分かつているときには、対応する検
出器抵抗F1ないしF2の抵抗値Rf1ないしRf2
直ちに算出される。何らかの外的状況により、例
えば電流Iの変化により、特性曲線が変化して
も、検出器抵抗の抵抗値は正しい値に保たれる。
FIG. 3 shows the course of the calibrated resistance value R with respect to the voltage drop V. The illustrated characteristic curve K shows the calibration value versus R e1 /
When two of V e1 and R e2 /V e2 and R d /V d are used, how they are expressed based on the data used will be shown. Furthermore, under the measurement voltage effect V f1
When V f2 is known, the resistance value R f1 or R f2 of the corresponding detector resistance F1 or F2 is immediately calculated. Even if the characteristic curve changes due to some external circumstances, for example due to a change in the current I, the resistance value of the detector resistor remains at the correct value.

例えば第3図に示すデータから、特性曲線Kの
勾配に関して次のような式が得られる。
For example, from the data shown in FIG. 3, the following equation regarding the slope of the characteristic curve K can be obtained.

Rf1−Re/Vf1−Ve=Rd/Vd (1) この式から簡単な変形によつて特許請求の範囲第
2項記載の式 Rf1=Re+(Vf1−Ve)Rd/Vd が得られる。
R f1 −R e /V f1 −V e =R d /V d (1) By simple modification of this formula, the formula R f1 =R e +(V f1 −V e ) R d /V d is obtained.

差形成の際にも次式が成立つ。 The following equation also holds true when forming a difference.

Rf1−Rf2/Vf1−Vf2=Rd/Vd (2) この式から特許請求の範囲第4項記載の式 Rf1−Rf2=(Vf1−Vf2)Rd/Vd が導出される。 R f1 −R f2 /V f1 −V f2 =R d /V d (2) From this formula, the formula recited in claim 4: R f1 −R f2 = (V f1 −V f2 )R d /V d is derived.

従つて差形成の際は単に特性曲線Kの勾配のみ
が問題であり、単に、差抵抗Dに注目さればよ
い。基準抵抗Gは省かれる。従つて差抵抗Dの許
容偏差を考慮しさえすればよく、この許容偏差に
ついても、測定電圧降下の差Vf1−Vf2の差抵抗に
おける較正電圧降下Vdに対する関係についての
み考慮しさえすればよい。
Therefore, when forming a difference, only the slope of the characteristic curve K matters, and it is only necessary to pay attention to the difference resistance D. The reference resistance G is omitted. Therefore, it is only necessary to take into account the tolerance of the differential resistance D, and regarding this tolerance only the relationship of the measured voltage drop difference V f1 −V f2 to the calibrated voltage drop V d across the differential resistance. good.

例えばPT100抵抗の場合に差較正値が50Ω±
0.01%で差領域が0〜130℃のとき、1℃は約380
mΩに相当する。差抵抗Dの全許容偏差は±5m
Ωである。これは差が130℃のとき0.013℃に相当
する。故に差が1℃のときの精度は0.0001℃/℃
である。従つて温度差が極めて小さい場合でも誤
差は問題にならなくなる。
For example, in the case of PT100 resistor, the difference calibration value is 50Ω±
When the difference range is 0 to 130℃ at 0.01%, 1℃ is approximately 380℃.
Corresponds to mΩ. Total tolerance of differential resistance D is ±5m
It is Ω. This corresponds to 0.013°C when the difference is 130°C. Therefore, when the difference is 1℃, the accuracy is 0.0001℃/℃
It is. Therefore, even if the temperature difference is extremely small, errors will not be a problem.

以上述べた装置は温度測定の別の用途にも用い
ることができ、例えば海運装置および工業装置に
おけるプロセツサの監視・制御用にも用いること
ができる。
The device described above can also be used for other applications of temperature measurement, for example for monitoring and controlling processors in maritime and industrial equipment.

また別の温度に依存する抵抗、例えばニツケル
センサを用いてもよい。
Other temperature dependent resistors may also be used, for example nickel sensors.

発明の効果 本発明の装置では温度測定信号変換器が必要な
い。むしろ検出器温度に対する重要な尺度となる
信号は検出器抵抗での電圧降下として直接得られ
る。較正電圧降下と記憶された較正値とから形成
される較正曲線に基づいて換算することにより、
検出器抵抗の極めて正確な抵抗値が得られ、この
値から相応に正確に測定すべき温度が検出され
る。最初に、較正に用いられる固定抵抗の抵抗
値、即ち較正値を正確に記憶しておけば充分であ
る。こうすれば動作中装置が自動的に調整され
る。すべての抵抗に同じ電流が流れるので、殊
に、電圧降下をもたらす電流の変動は全く問題に
ならない。
Effects of the Invention The device of the invention does not require a temperature measurement signal converter. Rather, a signal that is an important measure of the detector temperature is obtained directly as a voltage drop across the detector resistance. By converting based on a calibration curve formed from a calibrated voltage drop and a stored calibration value,
A very precise resistance value of the detector resistor is obtained, from which the temperature to be measured can be detected with corresponding precision. Initially, it is sufficient to accurately memorize the resistance value of the fixed resistor used for calibration, ie the calibration value. This will automatically adjust the device during operation. Since the same current flows through all resistors, in particular, current fluctuations that result in voltage drops are not a problem at all.

このようにして温度差、例えば供給流温度と戻
り流温度との差を求めようとする場合、極めて大
きな利点が得られる。つまり差形成の際に1つの
較正抵抗を完全にまたは事実上完全に無視するこ
とができるので、計算結果に他方の較正抵抗の許
容偏差しか影響せず、しかも全許容偏差の数分の
1の、つまりこの較正抵抗の全温度範囲に対する
温度差の比での偏差しか影響しない。
Significant advantages are obtained in this way when determining the temperature difference, for example the difference between the supply stream temperature and the return stream temperature. This means that one calibration resistor can be completely or virtually completely ignored during the difference formation, so that only the tolerance of the other calibration resistor influences the calculation result, and only a fraction of the total tolerance. , that is, only the deviation in the ratio of the temperature difference over the entire temperature range of this calibration resistor affects.

特許請求の範囲第2項記載の構成により、検出
器抵抗の実抵抗値を3つの測定された電圧降下と
2つの記憶された較正値とから得ることができ
る。このようにして得られた実抵抗値から通常の
方法で検出器抵抗の温度を算出でき、これは検出
器温度と検出器抵抗との間に直線的関係がなくて
も行なえる。
With the arrangement according to claim 2, the actual resistance value of the detector resistance can be obtained from three measured voltage drops and two stored calibration values. The temperature of the detector resistance can be calculated in the usual way from the actual resistance value thus obtained, and this can be done even if there is no linear relationship between the detector temperature and the detector resistance.

従つて少なくとも1つの検出器抵抗を、その抵
抗値が温度の自乗に依存するPT100抵抗により構
成することができる。
The at least one detector resistor can therefore be constituted by a PT100 resistor whose resistance value depends on the square of the temperature.

簡単には特許請求の範囲第4項記載の構成で充
分である。実際の検出器抵抗の抵抗値の差を形成
するので、換算は較正値とこれに対応する較正電
圧降下またはその等価量のみ用いて行なえばよ
い。このような簡易化は、検出器抵抗と温度とが
互いに直線的に依存するときかまたはこの直線性
からのずれが殊に温度差の小さいときはほとんど
問題にならないときに、可能である。
Simply speaking, the configuration described in claim 4 is sufficient. Since it forms the difference in the resistance value of the actual detector resistance, the conversion need only be performed using the calibration value and the corresponding calibration voltage drop or its equivalent. Such a simplification is possible when detector resistance and temperature are linearly dependent on each other or when deviations from this linearity are of little concern, especially at small temperature differences.

特許請求の範囲第5項記載の構成により、測定
された電圧降下を直接且つ簡単な方法で評価回路
に供給することができる。
The arrangement according to claim 5 makes it possible to supply the measured voltage drop to the evaluation circuit directly and in a simple manner.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は較正抵抗と検出器抵抗との直列接続の
回路図、第2図は熱交換器中で伝達された熱量を
測定する装置のための評価回路のブロツク回路
図、第3図は較正曲線図である。 F1,F2……検出器抵抗、G……基準抵抗、
D……差抵抗、1……電流源、12……較正値記
憶装置、14……評価回路、K……較正曲線。
Figure 1 is a circuit diagram of the series connection of a calibration resistor and a detector resistor, Figure 2 is a block diagram of an evaluation circuit for a device for measuring the amount of heat transferred in a heat exchanger, and Figure 3 is a circuit diagram of a series connection of a calibration resistor and a detector resistor. It is a curve diagram. F1, F2...Detector resistance, G...Reference resistance,
D...Differential resistance, 1...Current source, 12...Calibration value storage device, 14...Evaluation circuit, K...Calibration curve.

Claims (1)

【特許請求の範囲】 1 少なくとも1つの温度に依存する検出器抵抗
と、検出器抵抗の温度に依存する電圧降下を処理
する評価回路とを用いて温度値を測定する装置に
おいて、少なくとも1つの検出器抵抗F1,F2
が2つの固定較正抵抗、即ち基準抵抗Gおよび差
抵抗Dと共に直列接続にて共通の電流源1に接続
されており、基準抵抗は、所定の低い温度のとき
に検出器抵抗が示す最小較正値(Re1)を有して
おり、また差抵抗の差較正値(Rd)は、検出器
抵抗が所定の高い温度のときに示す最大較正値
(Re2)を較正抵抗の直列接続が有するような大
きさになつており、較正値記憶装置12が設けら
れており、較正抵抗のうちの少なくとも1つない
しは複数の較正抵抗の直列接続において少なくと
も1つの較正電圧降下(Ve1,Ve2,Vd)を検出
可能であり、また検出器抵抗において各々1つの
測定電圧降下(Vf1,Vf2)を検出可能であり、評
価回路14が実際温度値を少なくとも1つの測定
電圧降下から、少なくとも1つの較正値とこれに
対応する較正電圧降下とから形成される較正曲線
Kに基づいて検出することを特徴とする温度測定
装置。 2 評価回路14が式Rf1=Re+(Vf1−Ve)Rd/Vd により算出された検出器抵抗F1の実際の抵抗値
から実際の検出器温度を検出し、ただしRf1は検
出器抵抗の実際の抵抗値Vf1は検出器抵抗での電
源電圧降下、Reは最小または最大較正値、Ve
対応する較正電圧降下、Rdは差較正値すなわち
最大較正値と最小較正値との差、Vdは差較正値
に対応する較正電圧降下ないし対応する較正電圧
降下の差、である特許請求の範囲第1項記載の温
度測定装置。 3 少なくとも1つの検出器抵抗F1,F2が
PT100抵抗である特許請求の範囲第2項記載の温
度測定装置。 4 評価回路14が式Rf1−Rf2=(Vf1−Vf2)Rd/Vd により算出された2つの検出器抵抗F1,F2の
抵抗値差から実際の温度差を検出し、ただし Rf1は第1の検出器抵抗の実際の抵抗値、 Vf1は第1の検出器抵抗の測定電圧降下、 Rf2は第2の検出器抵抗の実際の抵抗値、 Vf2は第2の検出器抵抗の測定電圧降下、 Rdは差較正値ないし最大較正値と最小較正値
との差、 Vdは差較正値に対応する較正電圧降下ないし
較正電圧降下の差、 である特許請求の範囲第1項記載の温度測定抵
抗。 5 直列接続の抵抗G,D、F1,F2に設けら
れた電圧降下タツプが時間的に順次評価回路14
のマルチプレクサ13の入力側に接続され、さら
に評価回路がこの電圧降下用の中間記憶装置11
を有する特許請求の範囲第1項から第4項までの
いずれかに記載の温度測定装置。 6 評価回路がA−D変換器とデイジタル計算回
路とを備えており、該デイジタル計算回路が、熱
交換装置の供給流温度と戻り流温度との間の差
と、測定された流量と、1つの温度に依存する温
度係数とから伝達された熱量を算出し、前記デイ
ジタル計算回路8がさらに検出器抵抗F1,F2
の実際の抵抗値の算出および温度値への換算も行
う特許請求の範囲第1項記載の温度測定装置。
[Claims] 1. A device for measuring a temperature value using at least one temperature-dependent detector resistance and an evaluation circuit that processes a temperature-dependent voltage drop across the detector resistance, resistance F1, F2
is connected in series to a common current source 1 with two fixed calibration resistors, namely a reference resistor G and a differential resistor D, the reference resistor being the minimum calibrated value exhibited by the detector resistance at a given low temperature. (R e1 ), and the differential calibration value (R d ) of the differential resistance is such that the series connection of the calibration resistors has the maximum calibration value (R e2 ) that the detector resistance exhibits when it is at a predetermined high temperature. A calibration value storage device 12 is provided and at least one calibration voltage drop (V e1 , V e2 , V d ) and one measured voltage drop (V f1 , V f2 ) in each case across the detector resistance, the evaluation circuit 14 determines the actual temperature value from at least one measured voltage drop. A temperature measuring device characterized in that detection is based on a calibration curve K formed from at least one calibration value and a corresponding calibration voltage drop. 2. The evaluation circuit 14 detects the actual detector temperature from the actual resistance value of the detector resistor F1 calculated by the formula R f1 = R e + (V f1 − V e ) R d /V d , where R f1 is the actual resistance of the detector resistor, V f1 is the supply voltage drop across the detector resistor, R e is the minimum or maximum calibrated value, V e is the corresponding calibrated voltage drop, and R d is the difference or maximum calibrated value. 2. The temperature measuring device according to claim 1, wherein the difference from the minimum calibration value, Vd , is a calibration voltage drop corresponding to the differential calibration value or a difference between the corresponding calibration voltage drops. 3 At least one detector resistor F1, F2 is
The temperature measuring device according to claim 2, which is a PT100 resistor. 4. The evaluation circuit 14 detects the actual temperature difference from the resistance value difference between the two detector resistors F1 and F2 calculated by the formula R f1 - R f2 = (V f1 - V f2 ) R d /V d , but R f1 is the actual resistance value of the first detector resistor, V f1 is the measured voltage drop across the first detector resistor, R f2 is the actual resistance value of the second detector resistor, V f2 is the actual resistance value of the second detector resistor, The measured voltage drop across the detector resistance, R d is the difference between the differential calibration value or the maximum calibration value and the minimum calibration value, and V d is the calibration voltage drop or the difference between the calibration voltage drops corresponding to the differential calibration value. Temperature measuring resistor according to range 1. 5 The voltage drop taps provided on the series-connected resistors G, D, F1, and F2 are sequentially evaluated in time by the evaluation circuit 14.
The evaluation circuit is connected to the input side of the multiplexer 13 of
A temperature measuring device according to any one of claims 1 to 4. 6. The evaluation circuit comprises an analog-to-digital converter and a digital calculation circuit, the digital calculation circuit determining the difference between the supply stream temperature and the return stream temperature of the heat exchanger, the measured flow rate, and 1 The digital calculation circuit 8 further calculates the amount of heat transferred from the temperature coefficient that depends on the two temperatures, and the digital calculation circuit 8 further calculates the amount of heat transferred from the
2. The temperature measuring device according to claim 1, which also calculates an actual resistance value and converts it into a temperature value.
JP17690384A 1983-08-27 1984-08-27 Temperature measuring device Granted JPS6071925A (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
DE19833330915 DE3330915C2 (en) 1983-08-27 1983-08-27 Device for determining a temperature value by means of at least one temperature-dependent sensor resistor
DE3330915.9 1983-08-27

Publications (2)

Publication Number Publication Date
JPS6071925A JPS6071925A (en) 1985-04-23
JPH0338535B2 true JPH0338535B2 (en) 1991-06-11

Family

ID=6207574

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17690384A Granted JPS6071925A (en) 1983-08-27 1984-08-27 Temperature measuring device

Country Status (5)

Country Link
JP (1) JPS6071925A (en)
CA (1) CA1213672A (en)
DE (1) DE3330915C2 (en)
DK (1) DK163610C (en)
SE (1) SE8403843L (en)

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3808475A1 (en) * 1988-03-14 1989-10-19 Friedhelm Meyer Method and device to measure a temperature
DE19637561C1 (en) * 1996-09-14 1998-02-26 Dienes Apparatebau Gmbh Sensorless temperature control of a heating device
FR2874692B1 (en) * 2004-08-27 2006-10-13 Actaris Sas Soc Par Actions Si DEVICE FOR MEASURING TEMPERATURE IN A THERMAL ENERGY COUNTER
DE102005029319A1 (en) * 2005-06-24 2006-12-28 Abb Patent Gmbh Circuit arrangement, for determining temperature difference between two sensors, has digital microprocessor to determine temperature difference from digitized signals of analog-to-digital converter and provide temperature difference signal
JP5579097B2 (en) * 2011-02-16 2014-08-27 アズビル株式会社 4-wire RTD input circuit
DE102017130135A1 (en) 2017-12-15 2019-06-19 Endress + Hauser Wetzer Gmbh + Co. Kg Condition monitoring of a temperature sensor
CN110220606B (en) * 2019-06-24 2021-09-14 宁波华仪宁创智能科技有限公司 Temperature measuring device with calibration function and method

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DD206176A3 (en) * 1981-04-22 1984-01-18 METHOD AND CIRCUIT ARRANGEMENT FOR TEMPERATURE MEASUREMENT

Also Published As

Publication number Publication date
SE8403843D0 (en) 1984-07-24
SE8403843L (en) 1985-02-28
JPS6071925A (en) 1985-04-23
DK163610C (en) 1992-08-10
DE3330915C2 (en) 1986-09-04
DK400784A (en) 1985-02-28
DK163610B (en) 1992-03-16
CA1213672A (en) 1986-11-04
DE3330915A1 (en) 1985-03-14
DK400784D0 (en) 1984-08-22

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