JPH07218324A - Electronic balance - Google Patents

Electronic balance

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Publication number
JPH07218324A
JPH07218324A JP930494A JP930494A JPH07218324A JP H07218324 A JPH07218324 A JP H07218324A JP 930494 A JP930494 A JP 930494A JP 930494 A JP930494 A JP 930494A JP H07218324 A JPH07218324 A JP H07218324A
Authority
JP
Japan
Prior art keywords
resistor
current
coil
resistance
heat
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.)
Pending
Application number
JP930494A
Other languages
Japanese (ja)
Inventor
Toshiyuki Yamaguchi
敏之 山口
Akira Kawamoto
晟 河本
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.)
Shimadzu Corp
Original Assignee
Shimadzu Corp
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 Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP930494A priority Critical patent/JPH07218324A/en
Publication of JPH07218324A publication Critical patent/JPH07218324A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】 【目的】 フォースコイルに流れる電流(コイル電流)
を電圧信号に変換するための基準抵抗が数ppm程度の
温度係数を持っていても、コイル電流に正確に比例した
電圧信号を得ることができ、安価な基準抵抗を用いて高
精度化を達成することのできる電子天びんを提供する。 【構成】基準抵抗7に対して熱抵抗が略零の位置関係で
発熱用抵抗13を配置するとともに、この発熱用抵抗1
3に流す電流iをコイル電流Iの大きさに基づいて制御
する回路手段14を設け、コイル電流Iによる基準抵抗
7の発熱量と、発熱用抵抗13の発熱量との和が略一定
となるように発熱用抵抗13に流れる電流iを制御す
る。
(57) [Abstract] [Purpose] Current flowing in force coil (coil current)
Even if the reference resistance for converting the voltage signal to a voltage signal has a temperature coefficient of about several ppm, a voltage signal that is accurately proportional to the coil current can be obtained, and high precision is achieved by using an inexpensive reference resistance. Provide an electronic balance that can be used. [Structure] The heat generating resistor 13 is arranged in a positional relationship where the heat resistance is substantially zero with respect to the reference resistor 7, and the heat generating resistor 1 is arranged.
The circuit means 14 for controlling the current i flowing through 3 based on the magnitude of the coil current I is provided, and the sum of the heat generation amount of the reference resistor 7 and the heat generation amount of the heat generation resistor 13 due to the coil current I becomes substantially constant. Thus, the current i flowing through the heating resistor 13 is controlled.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は電磁力平衡型の電子天び
んに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electromagnetic force balance type electronic balance.

【0002】[0002]

【従来の技術】電磁力平衡型の電子天びんでは、一般
に、永久磁石による磁界中に可動のフォースコイルを配
置するとともに、このフォースコイルにレバー等を介し
て秤量皿を連結した機構を持ち、被測定荷重が秤量皿に
作用することによるレバー等の変位を変位センサで検出
して、その変位が零になるようにフォースコイルに流れ
る電流を制御する。そして、そのフォースコイルに流れ
る電流の大きさから、被測定荷重を算出するようになっ
ている。
2. Description of the Related Art In general, an electromagnetic force balance type electronic balance has a movable force coil arranged in a magnetic field of a permanent magnet and a mechanism in which a weighing dish is connected to the force coil via a lever or the like. The displacement sensor detects the displacement of the lever or the like due to the measurement load acting on the weighing pan, and the current flowing through the force coil is controlled so that the displacement becomes zero. Then, the load to be measured is calculated from the magnitude of the current flowing through the force coil.

【0003】ここで、フォースコイルに流れる電流の大
きさから表示器に表示すべき計量値を求めるに当たって
は、実際には、コイル電流を基準抵抗に流すことによっ
てアナログ電圧信号に変換した後、その電圧信号をA−
D変換器によってデジタル化し、これを荷重データとし
てマイクロコンピュータに採り込み、平均化処理等を施
して表示すべき計量値を得ている。
Here, in determining the measured value to be displayed on the display device from the magnitude of the current flowing through the force coil, in practice, the coil current is converted into an analog voltage signal by flowing it through a reference resistor, and then the analog voltage signal is converted. A-
The data is digitized by a D converter, loaded into a microcomputer as load data, subjected to averaging processing, etc. to obtain a measured value to be displayed.

【0004】[0004]

【発明が解決しようとする課題】ところで、以上のよう
な従来の電子天びんのうち、高精度のものにおいては、
基準抵抗として温度係数ができるだけ零に近いもので、
しかも許容電力が実際に使用される電力に比して数倍な
いし数十倍のものを使用する必要がある。
By the way, among the conventional electronic balances as described above, the ones with high precision are as follows:
The temperature coefficient of the reference resistance is as close to zero as possible,
Moreover, it is necessary to use the allowable power which is several times to several tens of times higher than the actually used power.

【0005】すなわち、基準抵抗はそこに流れるコイル
電流により発熱し、その温度が変化するが、この温度変
化によって基準抵抗の抵抗値が変化してしまうと、正し
くコイル電流を表す荷重データを得ることができない。
そこで、基準抵抗としては温度係数が可能な限り零に近
いもので、しかも許容電力が大きい抵抗体を使用して、
コイル電流が流れることによる温度変化を少なくし、ま
た、温度変化があっても抵抗値が変化しにくいものを使
用しなければならない。
That is, the reference resistance generates heat due to the coil current flowing therethrough, and its temperature changes, but if the resistance value of the reference resistance changes due to this temperature change, load data representing the coil current can be obtained correctly. I can't.
Therefore, as the reference resistance, use a resistor whose temperature coefficient is as close to zero as possible and has a large allowable power.
It is necessary to reduce the temperature change due to the coil current flowing, and to use the one whose resistance value does not easily change even if the temperature changes.

【0006】ここで、電子天びんの高精度化を追求して
いくためには、基準抵抗として温度係数が零のものが必
要となるが、絶対零の温度係数を持つ抵抗体は実質的に
は存在せず、この点が天びんの高精度化の限界となる。
また、絶対零ではなくても可能な限り零に近い抵抗体
で、しかも許容電力の大きいものを用いる場合でも、そ
のコストが高いという問題がある。
Here, in order to pursue high precision of the electronic balance, it is necessary to have a reference resistance having a temperature coefficient of zero, but a resistor having a temperature coefficient of absolute zero is substantially used. This does not exist, and this point is the limit for improving the precision of the balance.
Further, there is a problem that the cost is high even when a resistor which is not absolute zero but is as close to zero as possible and has a large allowable power is used.

【0007】本発明はこのような実情に鑑みてなされた
もので、基準抵抗の温度係数が数ppm程度あって、ま
た、許容電力がさほど大きくなくても、コイル電流を正
確に表す荷重データを得ることができ、安価な基準抵抗
を用いて高精度化を達成することのできる電子天びんの
提供を目的としている。
The present invention has been made in view of such circumstances, and the load data accurately representing the coil current can be obtained even if the temperature coefficient of the reference resistance is about several ppm and the allowable power is not so large. It is an object of the present invention to provide an electronic balance that can be obtained and can achieve high accuracy by using an inexpensive reference resistor.

【0008】[0008]

【課題を解決するための手段】上記の目的を達成するた
めの構成を、実施例図面である図1を参照しつつ説明す
ると、本発明の電子天びんは、磁界中のフォースコイル
4に流れる電流を電圧信号に変換する基準抵抗7に対し
て熱抵抗が略零となるような位置に発熱用抵抗13を配
置するとともに、この発熱用抵抗13に流す電流をコイ
ル電流の大きさに基づいて制御する回路手段14を有
し、その回路手段14は、コイル電流が流れることによ
る基準抵抗7の発熱量と、発熱用抵抗13の発熱量との
和が略一定となるよう、発熱用抵抗13に流れる電流を
制御することによって特徴づけられる。
A structure for achieving the above object will be described with reference to FIG. 1 which is an embodiment drawing, and an electronic balance of the present invention has a current flowing through a force coil 4 in a magnetic field. The heating resistor 13 is arranged at a position where the thermal resistance becomes substantially zero with respect to the reference resistor 7 for converting the voltage signal into a voltage signal, and the current flowing through the heating resistor 13 is controlled based on the magnitude of the coil current. The circuit means 14 has a circuit means 14 for controlling the heat generation resistance 13 so that the sum of the heat generation quantity of the reference resistance 7 and the heat generation quantity of the heat generation resistance 13 due to the coil current flowing becomes substantially constant. Characterized by controlling the current flow.

【0009】[0009]

【作用】本発明は、基準抵抗7にコイル電流が流れるこ
とによる自己加熱に起因する温度変化分を、これと熱抵
抗がほぼ零となる位置関係で置かれた発熱用抵抗13の
発熱量を加減することによって、相殺的に解消しようと
するものである。
According to the present invention, the amount of change in temperature due to self-heating caused by the coil current flowing through the reference resistor 7 and the amount of heat generated by the heating resistor 13 placed in a positional relationship in which the thermal resistance becomes substantially zero are calculated. By adjusting the amount, it is intended to cancel each other out.

【0010】すなわち、基準抵抗7には被測定荷重Wの
大きさに比例したコイル電流が流れ、その電流の大きさ
に応じた発熱量のもとに温度が変化することになるが、
この基準抵抗7に対して熱抵抗がほぼ零となるように発
熱用抵抗13を配置し、両者の発熱量の和が常にほぼ一
定となるように発熱用抵抗13に流す電流を制御する
と、基準抵抗7の温度はコイル電流の大きさにかかわら
ず一定となる。従って、温度係数が数ppm程度の抵抗
体を基準抵抗7としても、自己加熱による温度変化が殆
ど生じないが故に、コイル電流に正確に比例する電圧信
号が得られる。
That is, a coil current proportional to the magnitude of the load W to be measured flows through the reference resistor 7, and the temperature changes according to the amount of heat generated according to the magnitude of the current.
If the heat generating resistor 13 is arranged so that the heat resistance becomes substantially zero with respect to the reference resistor 7, and the current flowing through the heat generating resistor 13 is controlled so that the sum of the heat generation amounts of both is always constant, The temperature of the resistor 7 becomes constant regardless of the magnitude of the coil current. Therefore, even if a resistor having a temperature coefficient of several ppm is used as the reference resistor 7, a temperature change due to self-heating hardly occurs, so that a voltage signal accurately proportional to the coil current can be obtained.

【0011】[0011]

【実施例】図1は本発明実施例の構成を示すブロック図
である。被測定荷重Wは秤量皿1上に載せられる。この
秤量皿1は、支点2aに支持されたレバー2の一端側に
連結されており、そのレバー2の先端部分の変位は変位
センサ3によって検出される。レバー2の他端側には巻
き枠4aが固着されており、その巻き枠4aにフォース
コイル4が巻回されている。
1 is a block diagram showing the configuration of an embodiment of the present invention. The measured load W is placed on the weighing dish 1. The weighing dish 1 is connected to one end side of a lever 2 supported by a fulcrum 2a, and the displacement of the tip portion of the lever 2 is detected by a displacement sensor 3. A winding frame 4a is fixed to the other end of the lever 2, and the force coil 4 is wound around the winding frame 4a.

【0012】変位センサ3の出力はPID制御回路5に
導入され、このPID制御回路5では、変位センサ3の
出力の大きさに応じた電流をフォースコイル4に流す。
フォースコイル4は永久磁石を主体とする磁気回路6が
作る静磁界中に配置されており、PID制御回路5から
の電流がフォースコイル4に電流が流れることによっ
て、その電流の大きさと磁場の強さに応じた電磁力が発
生する。この電磁力はフォースコイル4および巻き枠4
aを介してレバー2に伝達され、被測定荷重Wに抗して
レバー2の変位が零となるように作用して系を平衡させ
る。従って、系の平衡状態においてフォースコイル4に
流れる電流の大きさは、磁気回路6による磁場の強さが
一定であれば被測定荷重Wに比例したものとなる。
The output of the displacement sensor 3 is introduced into the PID control circuit 5, and in this PID control circuit 5, a current corresponding to the magnitude of the output of the displacement sensor 3 is passed through the force coil 4.
The force coil 4 is arranged in a static magnetic field created by a magnetic circuit 6 mainly composed of a permanent magnet, and when the current from the PID control circuit 5 flows through the force coil 4, the magnitude of the current and the strength of the magnetic field are increased. An electromagnetic force corresponding to the strength is generated. This electromagnetic force is applied to the force coil 4 and the winding frame 4.
It is transmitted to the lever 2 via a and acts so that the displacement of the lever 2 becomes zero against the measured load W to balance the system. Therefore, in the equilibrium state of the system, the magnitude of the current flowing through the force coil 4 is proportional to the measured load W if the strength of the magnetic field by the magnetic circuit 6 is constant.

【0013】フォースコイル4に流れる電流は基準抵抗
7に流され、ここで電圧信号に変換された後にA−D変
換器8に導入される。A−D変換器8からのデジタルデ
ータは、従って、フォースコイル4に流れる電流の大き
さ、ひいては秤量皿1に作用する被測定荷重Wの大きさ
を表すデータ、つまり荷重データとなってマイクロコン
ピュータ9に採り込まれる。
The current flowing through the force coil 4 is passed through the reference resistor 7, converted into a voltage signal here, and then introduced into the AD converter 8. Therefore, the digital data from the A / D converter 8 becomes data representing the magnitude of the current flowing through the force coil 4 and, in turn, the magnitude of the measured load W acting on the weighing pan 1, that is, load data, and becomes a microcomputer. Adopted in 9.

【0014】マイクロコンピュータ9は荷重データのほ
かに、前記した磁気回路6内の永久磁石の近傍に置かれ
た温度センサ10からの温度検出信号をA−D変換器1
1でデジタル化した温度データをも採り込んでおり、こ
の温度データを用いて、永久磁石の温度変化に起因する
磁場変化を補償しつつ、荷重データを平均化する等によ
って表示器12に表示すべき計量値を決定する。
In addition to the load data, the microcomputer 9 uses the AD converter 1 to detect the temperature detection signal from the temperature sensor 10 placed near the permanent magnet in the magnetic circuit 6.
The temperature data digitized in 1 is also incorporated, and the temperature data is used to compensate the magnetic field change caused by the temperature change of the permanent magnet, and the load data is displayed on the display 12 by averaging the load data. Determine the weight value to be measured.

【0015】さて、基準抵抗7に近接して、この基準抵
抗7との熱抵抗がほぼ零となるような位置関係で、発熱
用抵抗13が設けられている。そしてこの発熱用抵抗1
3には、演算回路14から供給される電流iが流され
る。この電流iは、基準抵抗7に流れる電流であるコイ
ル電流Iの大きさに応じて演算回路14によって一意的
に求められる。
A heating resistor 13 is provided close to the reference resistor 7 in such a positional relationship that the thermal resistance with the reference resistor 7 becomes substantially zero. And this heating resistor 1
A current i supplied from the arithmetic circuit 14 is passed through 3. This current i is uniquely obtained by the arithmetic circuit 14 according to the magnitude of the coil current I which is the current flowing through the reference resistor 7.

【0016】すなわち、演算回路14は、PID制御回
路5の出力であるコイル電流Iを入力し、このコイル電
流Iと、基準抵抗7の抵抗値R、および発熱用抵抗13
の抵抗値R´とから、電流Iが流れることによる基準抵
抗7の発熱量と、電流iが流れることによる発熱用抵抗
13の発熱量との和が一定となるよう、その電流iの大
きさを決定する。式で表せば、
That is, the arithmetic circuit 14 receives the coil current I, which is the output of the PID control circuit 5, and inputs the coil current I, the resistance value R of the reference resistor 7, and the heating resistor 13.
Magnitude of the current i such that the sum of the heat generation amount of the reference resistor 7 due to the current I flowing and the heat generation amount of the heat generating resistor 13 due to the current i flowing becomes constant from the resistance value R ′ of To decide. Expressed as a formula,

【0017】[0017]

【数1】 [Equation 1]

【0018】となるような電流iを算出して、発熱用抵
抗13に供給する。つまり、演算回路14は、コイル電
流Iから
A current i that satisfies the above condition is calculated and supplied to the heating resistor 13. That is, the arithmetic circuit 14 calculates from the coil current I

【0019】[0019]

【数2】 [Equation 2]

【0020】によって電流iを演算し、発熱用抵抗13
に流す。その結果、基準抵抗7に流れる電流Iの大きさ
に関わらず、この基準抵抗7と発熱用抵抗13の発熱量
の和は常に一定となり、また、これら両者は熱抵抗がほ
ぼ零となるような位置関係で配置されているため、両者
の発熱量の和を適当な値に設定しておくことにより、こ
れら両者の温度は一定に保たれる。
The current i is calculated by
Shed on. As a result, regardless of the magnitude of the current I flowing through the reference resistor 7, the sum of the amounts of heat generated by the reference resistor 7 and the heat-generating resistor 13 is always constant, and the thermal resistances of these two are almost zero. Since they are arranged in a positional relationship, the temperature of these two can be kept constant by setting the sum of the calorific values of both to an appropriate value.

【0021】従って、基準抵抗7として、数ppm程度
のある程度の大きさの温度係数を持つ抵抗体を用いて
も、A−D変換器8には常にフォースコイル4に流れる
電流Iに正確に比例した電圧信号が供給される。
Therefore, even if a resistor having a temperature coefficient of a certain magnitude of about several ppm is used as the reference resistor 7, the AD converter 8 is always exactly proportional to the current I flowing through the force coil 4. The supplied voltage signal is supplied.

【0022】なお、発熱用抵抗13の温度係数は任意で
あり、また、この発熱用抵抗13と基準抵抗7とを、熱
抵抗がほぼ零となるように配置する方法としては、例え
ば両者をセラミック抵抗とした場合には、基板上にこれ
らの抵抗7および13を相互に錯綜するようにパターニ
ングする方法、あるいは基準抵抗7に対して、コイル様
の発熱用抵抗13を巻きつけたり、線または板状の発熱
用コイル13を貼り付ける等の方法を採用することがで
きる。
The temperature coefficient of the heat generating resistor 13 is arbitrary, and as a method of disposing the heat generating resistor 13 and the reference resistor 7 so that the heat resistance becomes substantially zero, for example, both of them are made of ceramic. When the resistors are used, a method of patterning these resistors 7 and 13 on the substrate so as to be intricate with each other, or a coil-like heat-generating resistor 13 is wound around the reference resistor 7, or a line or plate shape is used. It is possible to adopt a method such as attaching the heat-generating coil 13 of FIG.

【0023】また、演算回路14による電流iの演算方
法として、上記したような厳密な演算ではなく、より簡
易な演算に代えることができる。例えば、基準抵抗7と
発熱用抵抗13の抵抗値をほぼ同一にしておくととも
に、演算回路14では、基準抵抗7に流れるコイル電流
Iの最大値(フルスケール電流,100%)としたと
き、この基準抵抗7と発熱用抵抗13に流れる電流の合
計が常にその最大値となるように、補数演算を行う方法
を採用することができる。この場合、抵抗の発熱量はそ
こに流れる電流の2乗に比例するから、両抵抗の発熱量
の和のコイル電流Iに対する関係は、コイル電流Iが零
の場合とフルスケール値の場合において両抵抗の発熱量
の和が一致し、コイル電流Iが50%の場合には両抵抗
の発熱量の和がこれよりも少なくなる、全体として下に
凸の放物線状の発熱量となるが、基準抵抗7のみを設け
た従来の電子天びんに比して、基準抵抗7の自己加熱に
よる温度変化は大幅に緩和される。
Further, the method of calculating the current i by the arithmetic circuit 14 can be replaced with a simpler calculation instead of the above-mentioned strict calculation. For example, when the resistance values of the reference resistor 7 and the heat generating resistor 13 are set to be substantially the same and the maximum value (full scale current, 100%) of the coil current I flowing in the reference resistor 7 is set in the arithmetic circuit 14, A method of performing a complement operation can be adopted so that the total of the currents flowing through the reference resistor 7 and the heating resistor 13 is always the maximum value. In this case, the amount of heat generated by the resistor is proportional to the square of the current flowing therethrough. Therefore, the relationship between the sum of the amounts of heat generated by both resistors and the coil current I depends on whether the coil current I is zero or the full-scale value. When the sum of the heat generation amounts of the resistors is the same and the coil current I is 50%, the sum of the heat generation amounts of the both resistors is smaller than this. Compared with the conventional electronic balance provided with only the resistor 7, the temperature change due to the self-heating of the reference resistor 7 is significantly reduced.

【0024】[0024]

【発明の効果】以上説明したように、本発明によれば、
フォースコイルに流れる電流を電圧信号に変換してA−
D変換器に供給するための基準抵抗に対して、熱抵抗が
略零となるような位置関係に発熱用抵抗を配置するとと
もに、その発熱用抵抗には、基準抵抗に流れるコイル電
流の大きさに基づき、当該発熱用抵抗と基準抵抗との発
熱量の和が略一定となるような電流を流すように構成し
ているから、秤量皿上の荷重の大きさに応じて基準抵抗
に流れるコイル電流の大きさが変化して、この基準抵抗
単独の発熱量が変化しても、発熱用抵抗はその変化分を
相殺するように発熱する結果、基準抵抗の温度はコイル
電流の大小に関係なく常に一定となる。
As described above, according to the present invention,
Convert the current flowing through the force coil into a voltage signal and
The heat generating resistor is arranged in such a positional relationship that the thermal resistance becomes substantially zero with respect to the reference resistor for supplying to the D converter, and the magnitude of the coil current flowing through the reference resistor is set in the heat generating resistor. On the basis of the above, since a current is made to flow so that the sum of the heat generation amounts of the heat generation resistance and the reference resistance becomes substantially constant, a coil that flows in the reference resistance according to the size of the load on the weighing pan. Even if the magnitude of the current changes and the amount of heat generated by the reference resistance alone changes, the heat-generating resistor generates heat to cancel the change, and the temperature of the reference resistance is independent of the coil current. It will always be constant.

【0025】従って、本発明の採用により、基準抵抗と
して、例えば数ppm等のある程度の大きさの温度係数
を持ち、しかも許容電力が実際の使用電力より僅かに大
きな安価な抵抗体を採用しても、コイル電流の変化によ
る温度変化が零ないしは殆ど生じないが故に、常にコイ
ル電流を正確に比例した電圧信号を得ることが可能とな
る。よって、従来のこの種の電子天びんに比して、同等
の性能を得るに当たってはコストを低減することができ
る。また、電子天びんの高性能を追求していくに当たっ
て、温度係数が絶対零の抵抗が存在しない限り避けられ
ない、基準抵抗の自己加熱に起因する誤差の発生、とい
う問題を解消することができた。
Therefore, by adopting the present invention, an inexpensive resistor having a temperature coefficient of a certain size, for example, several ppm, and an allowable power slightly larger than the actual power used is adopted as the reference resistance. However, since the temperature change due to the change of the coil current is zero or hardly occurs, it is possible to always obtain the voltage signal which is exactly proportional to the coil current. Therefore, compared to the conventional electronic balance of this type, the cost can be reduced in obtaining the same performance. Also, in pursuing the high performance of electronic balances, we were able to solve the problems that were unavoidable unless there was a resistance with a temperature coefficient of absolute zero, and the occurrence of errors due to self-heating of the reference resistance. .

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

【図1】本発明実施例の構成を示すブロック図FIG. 1 is a block diagram showing the configuration of an embodiment of the present invention.

【符号の説明】[Explanation of symbols]

1 秤量皿 2 レバー 3 変位センサ 4 フォースコイル 5 PID制御回路 6 磁気回路 7 基準抵抗 8 A−D変換器 9 マイクロコンピュータ 12 表示器 13 発熱用抵抗 14 演算回路 1 Weighing pan 2 Lever 3 Displacement sensor 4 Force coil 5 PID control circuit 6 Magnetic circuit 7 Reference resistance 8 A-D converter 9 Microcomputer 12 Display 13 Heat generation resistance 14 Arithmetic circuit

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 磁界中に置かれたコイルに電流を流すこ
とによって発生する電磁力を被測定荷重と平衡させると
ともに、そのコイル電流を基準抵抗に流すことによって
電圧信号に変換した後、A−D変換器でデジタル化して
荷重データを得る電子天びんにおいて、上記基準抵抗に
対して熱抵抗が略零となるような位置に発熱用抵抗が配
置されているとともに、この発熱用抵抗に流す電流を制
御する回路手段を有し、その回路手段は、コイル電流が
流れることによる上記基準抵抗の発熱量と、上記発熱用
抵抗の発熱量の和が略一定となるよう、当該発熱用抵抗
に流れる電流を制御することを特徴とする電子天びん。
1. An electromagnetic force generated by passing a current through a coil placed in a magnetic field is balanced with a load to be measured, and the coil current is passed through a reference resistance to be converted into a voltage signal, and then A- In an electronic balance that obtains load data by digitizing with a D converter, a heating resistor is arranged at a position where the thermal resistance is substantially zero with respect to the reference resistance, and the current flowing through this heating resistor is The circuit means has a control means, and the circuit means has a current flowing through the heating resistor so that the sum of the heating value of the reference resistor and the heating value of the heating resistor due to the coil current flowing becomes substantially constant. An electronic balance characterized by controlling the.
JP930494A 1994-01-31 1994-01-31 Electronic balance Pending JPH07218324A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP930494A JPH07218324A (en) 1994-01-31 1994-01-31 Electronic balance

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP930494A JPH07218324A (en) 1994-01-31 1994-01-31 Electronic balance

Publications (1)

Publication Number Publication Date
JPH07218324A true JPH07218324A (en) 1995-08-18

Family

ID=11716736

Family Applications (1)

Application Number Title Priority Date Filing Date
JP930494A Pending JPH07218324A (en) 1994-01-31 1994-01-31 Electronic balance

Country Status (1)

Country Link
JP (1) JPH07218324A (en)

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