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JPS6053448B2 - differential transformer - Google Patents
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JPS6053448B2 - differential transformer - Google Patents

differential transformer

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Publication number
JPS6053448B2
JPS6053448B2 JP51158338A JP15833876A JPS6053448B2 JP S6053448 B2 JPS6053448 B2 JP S6053448B2 JP 51158338 A JP51158338 A JP 51158338A JP 15833876 A JP15833876 A JP 15833876A JP S6053448 B2 JPS6053448 B2 JP S6053448B2
Authority
JP
Japan
Prior art keywords
winding
primary winding
windings
primary
secondary winding
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
JP51158338A
Other languages
Japanese (ja)
Other versions
JPS5383016A (en
Inventor
一郎 和田
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric Co Ltd
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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP51158338A priority Critical patent/JPS6053448B2/en
Publication of JPS5383016A publication Critical patent/JPS5383016A/en
Publication of JPS6053448B2 publication Critical patent/JPS6053448B2/en
Expired legal-status Critical Current

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  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
  • Transmission And Conversion Of Sensor Element Output (AREA)

Description

【発明の詳細な説明】 本発明は、大きな変位を精密に測定することのできる
差動トランスに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a differential transformer that can accurately measure large displacements.

従来の差動トランスは第1図(3段形)あるいは第2
図(2段形)に示す様な構成がとられており、その等価
回路は第3図の様になる。
Conventional differential transformers are shown in Figure 1 (3-stage type) or 2-stage type.
The configuration shown in the figure (two-stage type) is adopted, and its equivalent circuit is as shown in FIG.

すなわち、2個の2次巻線2a、2bを1次巻線1を挾
むように(第1図)又は1次巻線1の内側に(第2図)
互いに差動的関係に配置し、2次巻線2a、2bに誘起
する起電力の差が中間部に配置された鉄芯3の位置によ
つて変化することを利用して変位を測定するものである
。 ところで、このような従来例は、微小変位測定には
適しているが、大きな変位の測定には適当ではない。
That is, the two secondary windings 2a and 2b are placed between the primary winding 1 (Fig. 1) or inside the primary winding 1 (Fig. 2).
Displacement is measured by using the difference in electromotive force induced in the secondary windings 2a and 2b, which are arranged in a differential relationship with each other, depending on the position of the iron core 3 arranged in the middle. It is. By the way, such a conventional example is suitable for measuring minute displacements, but is not suitable for measuring large displacements.

すなわち、変位に対応して鉄芯3が動くため、1次巻線
1に対する磁束分布が第4図に示す様に偏移し、変位が
比較的大きくなると、2次巻線2a、2bに鎖交する磁
束と変位との間に直線的関係がなくなり、正しい出力が
得られない。
That is, since the iron core 3 moves in response to the displacement, the magnetic flux distribution to the primary winding 1 shifts as shown in FIG. There is no longer a linear relationship between the intersecting magnetic flux and displacement, and correct output cannot be obtained.

従つて、精密測定或は鉄芯の微小域であり、大きな変位
の精密測定は不可能である。 本発明は、従来の問題点
を解決するためになされたもので、大きな変位を精密に
測定することのできる差動トランスの提供を目的とする
Therefore, precision measurement is required in a minute area of the iron core, and precision measurement of large displacements is impossible. The present invention was made in order to solve the problems of the conventional art, and an object of the present invention is to provide a differential transformer that can accurately measure large displacements.

この目的を達成するために、本発明は、同一巻線数の
2つの巻線を差動的に結線し、かつ左右対称となるよう
に共軸配置して極性の異なる2つの磁界を発生させる1
次巻線と、この1次巻線と同軸的に配置されるとともに
軸方向に対称的位置変化が可能となるように重合されて
配置され、1次巻線との位置関係が相対的に変化するこ
とにより変化する1次巻線の各巻線との重合巻数に応じ
た出力を生じる2次巻線とを具備し、上記1次巻線によ
り極性の異なる2つの磁界を発生させ、前記1次巻線と
前記2次巻線との相対位置を前記2次巻線に誘起される
出力により検出するものである。
In order to achieve this objective, the present invention generates two magnetic fields with different polarities by differentially connecting two windings having the same number of windings and coaxially symmetrically arranging them. 1
The secondary winding is arranged coaxially with the primary winding and overlapped so that the position can be changed symmetrically in the axial direction, and the positional relationship with the primary winding can be changed relatively. and a secondary winding that generates an output according to the number of overlapping turns with each winding of the primary winding that changes by The relative position between the winding and the secondary winding is detected by the output induced in the secondary winding.

より具体的に述べれば、本発明は従来の様に2次巻線
を差動巻線とするのではなく、1次巻線を差動的に巻き
回して、この1次巻線に電流を流し、非差動的な2次巻
線に誘起される出力により1次巻線と2次巻線の相対位
置すなわち変位を検出するものである。
More specifically, the present invention winds the primary winding differentially, instead of making the secondary winding a differential winding as in the past, and passes current to the primary winding. The relative position or displacement of the primary winding and the secondary winding is detected by the output induced in the non-differential secondary winding.

1次巻線と2次巻線の相対位置は2次巻線の「等価的
巻線」に対応する。
The relative positions of the primary and secondary windings correspond to the "equivalent winding" of the secondary winding.

「等価的巻数」とは、第5図に示す様に差動的1次巻線
51の対称軸線XX″の左右に存在する2次巻線52a
,52b0,巻線をそれぞれA,Bとすると(A−B)
で表わされる。そして、第5図aのように変位がなけれ
ば、であり出力信号はA−B=0となる。
The "equivalent number of turns" refers to the secondary windings 52a that exist on the left and right sides of the axis of symmetry XX'' of the differential primary winding 51, as shown in FIG.
, 52b0, if the windings are A and B, respectively (A-B)
It is expressed as If there is no displacement as shown in FIG. 5a, then the output signal becomes A-B=0.

これが第5図Bf)Lに偏位dが生じると、となり、出
力信号はA−B〉0となり、変位dが検出される。
When a deviation d occurs in Bf)L in FIG. 5, the output signal becomes A-B>0, and the displacement d is detected.

すなわち、本発明の2次巻線は変位に対応して巻線が変
化する如く(可変巻線コイルの如く)動作する。また、
差動的1次巻線51は左右対称磁束を発生し、第5図b
の様に変位dが生じても、1次巻線51の磁束の分布自
体に偏移が生ずることはなく、2次巻線52に対する鎖
交磁束のみが変位に応じて変化し、2次巻線52の出力
は第5図の場合2次巻線の長さに対応する変位まで直線
的に変化し、大きな変位まで精密に測定することができ
る。以下、添附図面を参照して本発明の具体的実施例を
説明する。
That is, the secondary winding of the present invention operates so that the winding changes in response to displacement (like a variable winding coil). Also,
The differential primary winding 51 generates a symmetrical magnetic flux, as shown in FIG.
Even if a displacement d occurs as shown in FIG. The output of line 52 varies linearly in the case of FIG. 5 up to a displacement corresponding to the length of the secondary winding, and can be precisely measured up to large displacements. Hereinafter, specific embodiments of the present invention will be described with reference to the accompanying drawings.

第6図aは、空芯構造とし、同一巻線数の2つの1次巻
線61aと61Bをセパレータ63を介して左右対象に
共軸配置し、2次巻線62を1次巻線61a,61bの
の外側に同軸的に配置し、2次巻線62の中央が1次巻
線61a,61bの対称軸線に略一致するように構成し
たものである。
FIG. 6a shows an air-core structure in which two primary windings 61a and 61B having the same number of windings are coaxially arranged symmetrically on the left and right through a separator 63, and the secondary winding 62 is connected to the primary winding 61a. , 61b so that the center of the secondary winding 62 substantially coincides with the axis of symmetry of the primary windings 61a, 61b.

すなわち、この2次巻線は、1次巻線と同軸的に配置さ
れるとともに軸方向に対称的位置変化.が可能となるよ
うに重合されて配置され、1次巻線との位置関係が相対
的に変化することにより変化する1次巻線の各巻線との
重合巻数に応じた出力を生じるように構成されている。
磁路抵抗が高いので磁束が0となることがなく、2つの
1次巻I線61aと61bからなる差動1次巻線の磁束
が変位により変化せす大きな変位を精度良く測定できる
。なお、セパレータ63の長さ1は略0でもよく、ある
いは数〜数10Dでもよい。第6図bは2次巻線を所定
長分離された2つの′2次巻線62a,62bとし、こ
れらを非差動的に接続して構成したものである。
That is, the secondary winding is arranged coaxially with the primary winding and changes its position symmetrically in the axial direction. The windings are arranged in a superimposed manner so that the windings are overlapped with each other, and are configured to produce an output according to the number of turns of the primary winding that overlaps with each winding, which changes as the positional relationship with the primary winding changes relative to the primary winding. has been done.
Since the magnetic path resistance is high, the magnetic flux does not become 0, and it is possible to accurately measure the large displacement caused by the displacement of the magnetic flux of the differential primary winding consisting of the two primary winding I wires 61a and 61b. Note that the length 1 of the separator 63 may be approximately 0, or may be several to several 10D. FIG. 6b shows a configuration in which the secondary windings are two secondary windings 62a and 62b separated by a predetermined length and connected non-differentially.

この場合、1次巻線61aと61bの間の距離も2次巻
線62a,62bの間隔に応じたものに設定される。第
7図は、空芯構造とはせず、磁芯(例えば鉄芯、フェラ
イト等)を使用した本発明の実施例である。第7図にお
いて、1次巻線71aは磁芯14aに固定的に巻かれ、
1次巻線71aは磁芯74bに固定的に巻かれ、磁芯7
4aと74bは非磁性体75により結合されている。2
次巻線72は、1次巻線71a,71bの外側に同軸的
に配設され、2次巻線72の中央が1次巻線71a,7
1bの対称軸線に略一致するように構成され1る。
In this case, the distance between the primary windings 61a and 61b is also set according to the interval between the secondary windings 62a and 62b. FIG. 7 shows an embodiment of the present invention in which a magnetic core (eg, iron core, ferrite, etc.) is used instead of an air core structure. In FIG. 7, the primary winding 71a is fixedly wound around the magnetic core 14a,
The primary winding 71a is fixedly wound around the magnetic core 74b.
4a and 74b are coupled by a non-magnetic material 75. 2
The secondary winding 72 is disposed coaxially outside the primary windings 71a, 71b, and the center of the secondary winding 72 is located between the primary windings 71a, 71b.
1b is configured to substantially coincide with the axis of symmetry of 1b.

このように差動的1次巻線を磁芯に固定的に巻いても、
1次巻線の磁束が変位により変化することはなく、大き
な変位を精度良く測定できる。第8図は、2次巻線82
を1次巻線81a,81bの内側に設け、空芯構造とし
たものである。第6図のものと同様に、2つの1次巻線
81aと81bはセパレータ83により結合され、2次
巻線82の中央は1次巻線81aと81bの対称軸線に
略一致する。このようにしても、大きな変位を精度よく
測定できる。第9図は、第6図の実施例を半円形とした
もので、2次巻線92が、1次巻線91a,91bの外
側に配設され、2次巻線92の中央が1次巻線91a,
91bの対称軸線に略一致するように構成され、1次巻
線91aと91bがセパレータ93により結合される点
は第6図のものと同様である。
Even if the differential primary winding is fixedly wound around the magnetic core in this way,
The magnetic flux of the primary winding does not change due to displacement, and large displacements can be measured with high accuracy. FIG. 8 shows the secondary winding 82
is provided inside the primary windings 81a and 81b, and has an air-core structure. Similar to the one in FIG. 6, the two primary windings 81a and 81b are coupled by a separator 83, and the center of the secondary winding 82 substantially coincides with the axis of symmetry of the primary windings 81a and 81b. Even in this case, large displacements can be measured with high accuracy. FIG. 9 shows a semicircular version of the embodiment shown in FIG. 6, in which the secondary winding 92 is disposed outside the primary windings 91a and 91b, and the center of the secondary winding 92 is arranged in a semicircular manner. Winding wire 91a,
The primary windings 91a and 91b are connected by a separator 93, which is similar to that shown in FIG.

このように構成しても同様の効果がある。第10図は、
第7図の実施例を円形にしたものである。1次巻線10
1aと101bはそれぞれ磁芯104a,104bに固
定的に巻かれて非磁性体(例えばセラミック、樹脂等)
105を介して対称的に連結される。
Even with this configuration, similar effects can be obtained. Figure 10 shows
This is a circular version of the embodiment shown in FIG. Primary winding 10
1a and 101b are fixedly wound around magnetic cores 104a and 104b, respectively, and made of non-magnetic material (for example, ceramic, resin, etc.)
They are symmetrically connected via 105.

非磁性体105は磁気抵抗を大きくするために挿入され
る。1次巻線101aと101bの連結点にはセパレー
タ103が設けられるが、これは省略してもよい。2次
巻線102はその中央が1次巻線101a,101bの
対称軸線に一致するように配設される。
Nonmagnetic material 105 is inserted to increase magnetic resistance. A separator 103 is provided at the connection point between the primary windings 101a and 101b, but this may be omitted. The secondary winding 102 is arranged so that its center coincides with the axis of symmetry of the primary windings 101a, 101b.

帰還磁芯106は1次巻線101a,101bの内側に
帰還磁路の磁気抵抗を低くするために設けられる。この
ように構成しても同様の効果がある。なお、帰還磁芯を
省略してもよい。以上の説明から明らかな様に、本発明
による差動トランスは、同一巻線数の2つの巻線を差動
的に結線し、かつ左右対称となるように共軸配置して極
性の異なる2つの磁界を発生させる1次巻線と、この1
次巻線と同軸的に配置されるとともに軸方向に対称的位
置変化が可能となるように重合されて配置され、1次巻
線との位置関係が相対的に変化することにより変化する
1次巻線の各巻線との重合巻数に応じた出力を生じる2
次巻線とを具備し、1次巻線により極性が異なる2つの
磁界を発生させ、変位に関連する1次巻線と2次巻線の
相対位置を2次巻線に誘起される出力により検出するも
のであるから、差動的1次巻線の磁束が変位により変化
することはないので、大きな変位を精度良く測定できる
A feedback core 106 is provided inside the primary windings 101a and 101b in order to lower the magnetic resistance of the feedback magnetic path. Even with this configuration, similar effects can be obtained. Note that the feedback core may be omitted. As is clear from the above description, the differential transformer according to the present invention has two windings having the same number of windings differentially connected, and two windings having different polarities arranged coaxially so as to be symmetrical. A primary winding that generates two magnetic fields, and a primary winding that generates two magnetic fields.
The primary winding is arranged coaxially with the secondary winding and is arranged so as to be overlapped so that it can change its position symmetrically in the axial direction, and changes as the positional relationship with the primary winding changes relatively. Produces an output according to the number of overlapping turns with each winding of the winding 2
The primary winding generates two magnetic fields with different polarities, and the relative position of the primary winding and the secondary winding related to displacement is determined by the output induced in the secondary winding. Since the magnetic flux of the differential primary winding does not change due to displacement, large displacements can be measured with high accuracy.

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

第1図及び第2図は従来の差動トランスを示す断面図、
第3図は第2図の差動トランスの等価回路を示す回路図
、第4図は従来例の動作を示す説明図、第5図は本発明
の原理を示す説明図、第6図、第7図、第8図、第9図
及び第10図は本発明の実施例を示す断面図である。 1,11・・・・・・1次巻線、2a,2b,12a,
12b・・・・・・2次巻線、3,13・・・・・・鉄
芯、51a,51b,61a,61b,71a,71b
,81a,81b,91a,91b,101a,101
b,111a,111b・・・・・1次巻線、52,6
2,72,82,92,102,112,122・・・
・・・2次巻線、63,83,93,103,113・
・・・・セパレータ、74a,74b,104a,10
4b,114a,114b・・・・・・磁芯、75,1
05・・・・・非磁性体。
1 and 2 are cross-sectional views showing a conventional differential transformer,
3 is a circuit diagram showing an equivalent circuit of the differential transformer shown in FIG. 2, FIG. 4 is an explanatory diagram showing the operation of the conventional example, FIG. 5 is an explanatory diagram showing the principle of the present invention, 7, FIG. 8, FIG. 9, and FIG. 10 are cross-sectional views showing embodiments of the present invention. 1, 11...Primary winding, 2a, 2b, 12a,
12b... Secondary winding, 3, 13... Iron core, 51a, 51b, 61a, 61b, 71a, 71b
, 81a, 81b, 91a, 91b, 101a, 101
b, 111a, 111b...Primary winding, 52,6
2, 72, 82, 92, 102, 112, 122...
・・・Secondary winding, 63, 83, 93, 103, 113・
...Separator, 74a, 74b, 104a, 10
4b, 114a, 114b...Magnetic core, 75,1
05...Nonmagnetic material.

Claims (1)

【特許請求の範囲】[Claims] 1 同一巻線数の2つの巻線を差動的に結線し、かつ左
右対称となるように共軸配置して極性の異なる2つの磁
界を発生させる1次巻線と、この1次巻線と同軸的に配
置されるとともに軸方向に対称的位置変化が可能となる
ように重合されて配置され、1次巻線との位置関係が相
対的に変化することにより変化する1次巻線の各巻線と
の重合巻数に応じた出力を生じる2次巻線とを具備した
ことを特徴とする差動トランス。
1. A primary winding in which two windings with the same number of windings are connected differentially and coaxially arranged symmetrically to generate two magnetic fields with different polarities, and this primary winding. The primary winding is arranged coaxially with the primary winding and is arranged in a superimposed manner so that the position can be changed symmetrically in the axial direction, and changes as the positional relationship with the primary winding changes relative to the A differential transformer comprising a secondary winding that produces an output according to the number of overlapping turns with each winding.
JP51158338A 1976-12-28 1976-12-28 differential transformer Expired JPS6053448B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP51158338A JPS6053448B2 (en) 1976-12-28 1976-12-28 differential transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP51158338A JPS6053448B2 (en) 1976-12-28 1976-12-28 differential transformer

Publications (2)

Publication Number Publication Date
JPS5383016A JPS5383016A (en) 1978-07-22
JPS6053448B2 true JPS6053448B2 (en) 1985-11-26

Family

ID=15669442

Family Applications (1)

Application Number Title Priority Date Filing Date
JP51158338A Expired JPS6053448B2 (en) 1976-12-28 1976-12-28 differential transformer

Country Status (1)

Country Link
JP (1) JPS6053448B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6239947U (en) * 1985-04-24 1987-03-10

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4727316A (en) * 1985-04-16 1988-02-23 The United States Of America As Represented By The United States Department Of Energy Transformer current sensor for superconducting magnetic coils

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS532100B2 (en) * 1973-07-02 1978-01-25

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6239947U (en) * 1985-04-24 1987-03-10

Also Published As

Publication number Publication date
JPS5383016A (en) 1978-07-22

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