JPS6079281A - Magnetic sensor - Google Patents
Magnetic sensorInfo
- Publication number
- JPS6079281A JPS6079281A JP58187459A JP18745983A JPS6079281A JP S6079281 A JPS6079281 A JP S6079281A JP 58187459 A JP58187459 A JP 58187459A JP 18745983 A JP18745983 A JP 18745983A JP S6079281 A JPS6079281 A JP S6079281A
- Authority
- JP
- Japan
- Prior art keywords
- resin
- magnetic
- molded
- hall element
- flat plate
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/02—Measuring direction or magnitude of magnetic fields or magnetic flux
- G01R33/06—Measuring direction or magnitude of magnetic fields or magnetic flux using galvano-magnetic devices
- G01R33/07—Hall effect devices
Landscapes
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Measuring Magnetic Variables (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の技術分野〕
この発明は高い感度を有するホール素子等の磁気センサ
に関する。DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a magnetic sensor such as a Hall element having high sensitivity.
磁力を電気信号に変換する感磁素子の代表的なものとし
てホール素子がある。このホール素子における出力電圧
は第1図のような回路で測定されている。ボール素子1
oは図示するように直交する2つの辺を有し、−方の辺
の両<、、+:3 、t、5Jに所定の直l#、@流I
−i流し、他方の辺の両9i^1間にそのときの印加磁
束密度の大きさに比例した電圧を発生、出力するもので
あり、この出力電圧は増幅器1ノで増幅された後に測′
、i揚送1.る1、いま、ホール素子IOにおける八−
ヤリアの不多I′l史度をμ、ホール素子10の11f
b作71j流であるl二1;l:直流電流Iの値をIC
1上記電流を流すI61のホール素子10のインピーダ
ンスである人力iA抗の値をRd、印加磁束密度をBと
すると、ホール素子10の出力′に圧VHとこれらの値
との間には次のような比例関係が成立する。A Hall element is a typical example of a magnetically sensitive element that converts magnetic force into an electric signal. The output voltage of this Hall element is measured by a circuit as shown in FIG. Ball element 1
o has two orthogonal sides as shown in the figure, and both sides of the − side <, , +: 3, t, 5J have a predetermined angle l#, @flow I
−i, and generates and outputs a voltage proportional to the magnitude of the applied magnetic flux density at that time between both sides 9i^1 of the other side, and this output voltage is measured after being amplified by amplifier 1.
, i lift 1. 1. Now, 8- in Hall element IO
Yaria's Futai I'l history is μ, 11f of Hall element 10
b 71j current l21; l: The value of the DC current I is IC
1. If the value of the human force iA resistance, which is the impedance of the Hall element 10 of I61 through which the above current flows, is Rd, and the applied magnetic flux density is B, then the pressure VH at the output of the Hall element 10 and the relationship between these values are as follows. A proportional relationship holds true.
VHCX:μ・工。・Rd −B ・・・・・・・・・
(1)上記(1)式から明らかなように、I、 、 r
tdが一定であれば移動度μと磁束密度Bの値が大きい
(゛−高出力が得られる。したがい、従来では高出力を
得るために5μの値の大きなインジウムアンチモン(I
nSb )やガリウムヒ素(GaAs )などの材料を
用いてホール素子10を構成するようにしている。VHCX:μ・ENG.・Rd-B・・・・・・・・・
(1) As is clear from the above formula (1), I, , r
If td is constant, the values of mobility μ and magnetic flux density B are large (゛-high output can be obtained. Therefore, in the past, indium antimony (I
The Hall element 10 is constructed using a material such as nSb) or gallium arsenide (GaAs).
インジウムアンチモンを用いた従来のホール素子では単
結晶を作ることが困難であるので薄膜を利用せざるを得
す、このため素子安定性や信頼性が低くなるという欠点
がある。In conventional Hall elements using indium antimony, it is difficult to make a single crystal, so a thin film must be used, which has the disadvantage of lower element stability and reliability.
他方、ガリウムヒ素を用いたものは単結晶が比較的容易
に作れるので素子安定性や信頼性を高くすることができ
るが、反面、μの値がインジウムアンチモンを用いたも
のの1/1o以下と小さいので高出力を得ることができ
ず、高感度化が容易に達成できないという欠点がある。On the other hand, devices using gallium arsenide can make single crystals relatively easily and can improve device stability and reliability, but on the other hand, the value of μ is small, less than 1/1 of that using indium antimony. Therefore, high output cannot be obtained and high sensitivity cannot be easily achieved.
このように従来のホール素子では、素子安定性および信
頼性と高感度特性とを同時に満足するものがなく、いず
れが一方の特性t ’12−牲にしているのが実情であ
る。As described above, there is no conventional Hall element that satisfies both element stability and reliability as well as high sensitivity characteristics at the same time, and the reality is that one of them comes at the expense of the other.
〔発明の目的〕
この発明は上記のような事情を考慮してなされたもので
あシ、その目的は、素子安定性および信頼性と高感度特
性とを同時に満足する((&気センサを提供することに
ある。[Object of the Invention] The present invention has been made in consideration of the above-mentioned circumstances, and its purpose is to simultaneously satisfy element stability and reliability and high sensitivity characteristics. It's about doing.
この発明による磁気センサは、感磁素子をル磁性体樹脂
部材でまず平板状Vこ封止成型し、さらにこの非磁性体
樹脂部材をその、゛モ鵠両面から−lJ°ンドイッチ状
に挟持するように磁性体樹脂部劇を成型することによシ
集磁効果全高めで高+iC’T度化を図り、ガリウムヒ
素ケ用いた感磁、・i4子の感度死金達成できるように
したものである。In the magnetic sensor according to the present invention, a magneto-sensitive element is first molded into a flat plate shape with a magnetic resin member, and then this non-magnetic resin member is sandwiched between both sides of the non-magnetic resin member in a -lJ° sandwich shape. By molding the magnetic resin part, we have achieved a total magnetic collection effect and a high +iC'T degree, making it possible to achieve magnetic sensitivity using gallium arsenide and the sensitivity of I4. It is.
以下図面を参照してこの発明の一実施例を説明する。第
2図はこの発明に係る<a気センナ金ホール素子に実施
した場合の素子の外観全示す斜視図、第3図はその断面
図である。Iglにおいて21は、ガリウムヒ素からな
る絶縁基板を用い、この基板の表面領域にシリコンイオ
ンを選択的にイオン注入して前記第1図に示すような形
状のn型領域が形成されているホール素子チップである
。このチップ21は支持リード22上に半田もしくは接
着剤を用いて固定されている。また上記ホール素子チッ
プ2ノの表面上には、前記のような動作電流全供給する
だめの2つの入力電極および出力′[IL圧を外部に導
くための2つの出力電極が設けられており、これらチリ
20表面上の′磁極は金j((1線からたるポンディン
グワイヤ23を介して、4つの外部リード24ないし2
7と接続されている。さらに」二言己ホール素子チノン
o21は、上記yJ!ンf” 、(フグワイヤ23等と
ともに非磁性体の樹脂/Cとえば工・j?ギシ系樹脂2
8によっで封止され、この樹脂28は図示するように平
板状に成型さJl、る。さらVここの樹脂28は、図示
するようにその中火部すなわちホール素子チップ2ノに
対応する7445位が表裏両面とも内部に凹んプど形状
とされ、この部位の厚みが他の部位よりも薄く成型され
ている。。An embodiment of the present invention will be described below with reference to the drawings. FIG. 2 is a perspective view showing the entire external appearance of the <a-senna gold Hall element according to the present invention, and FIG. 3 is a sectional view thereof. In Igl, 21 is a Hall element in which an insulating substrate made of gallium arsenide is used, and silicon ions are selectively implanted into the surface region of the substrate to form an n-type region as shown in FIG. It's a chip. This chip 21 is fixed onto support leads 22 using solder or adhesive. Further, on the surface of the Hall element chip 2, two input electrodes for supplying the entire operating current as described above and two output electrodes for guiding the output '[IL pressure to the outside] are provided. The 'magnetic poles on the surface of these dusts 20 are connected to the four external leads 24 to 2 through the bonding wire 23 made of gold (1 wire).
7 is connected. In addition, the Hall element Chinon o21 is the same as the above yJ! f'', (with blow wire 23, etc., non-magnetic resin/C, for example, engineering/j? ginseng resin 2
8, and this resin 28 is molded into a flat plate shape as shown in the figure. As shown in the figure, the resin 28 here is shaped like an inward concave part on both the front and back surfaces at the middle heat part, i.e., the 7445th position corresponding to the Hall element chip 2, and the thickness of this part is thicker than the other parts. Molded thinly. .
上記樹脂28の表裏両面には、磁性体の樹脂たとえば工
月?キシ系樹脂にF e −N i系や”5− Z n
系のFe微粒子など透磁率が高い物質の砥粒子を混入し
た樹脂29が設けらノ゛シておシ、し/cがって上記樹
脂29は樹脂28をその表裏両面がらり“ンドイッチ状
に挾持するように成型さり、ている。Both the front and back surfaces of the resin 28 are made of magnetic resin, such as Kogetsu? F e -N i type and "5-Z n
The resin 29 mixed with abrasive particles of a material with high magnetic permeability such as Fe fine particles is not provided, and therefore, the resin 29 holds the resin 28 on both its front and back surfaces in a "nandwich" manner. It is molded to look like this.
このような構成でなるホールイベ子C[、外1I11j
の樹脂29が磁性体であるので、磁界中に置い7rとき
に磁束が十分に集められ電磁効果を高めることができる
。この/ζめ、前記(1)式における1市束密度が高め
られ、これにより高感)W化°を達成することができる
。なお、ホール素子チップ21全いったん非磁性体の樹
脂28を用いてJ3t +l: L、この両側にさらに
磁性体の樹脂29を成J−リしているのは、ガリウムヒ
素からなるポール素子チッ7′21が元々非磁性体で必
υ、全体音f社性体の樹脂で封止成型−j−ると、磁束
がチップ″21 ’i’、)S分を通らず樹脂部分を通
ってしまうからである、さらに上記実施例によ7’Lば
2非磁性体の樹j11128の厚みがチップ21に対応
しグこ部位で薄くなるように成型さiシているので、こ
の部位における磁気抵抗が最も小さくなる。このため、
i1之]11めることがてきる。Hall event child C [, outside 1I11j with such a configuration
Since the resin 29 is a magnetic material, when placed in a magnetic field, magnetic flux is sufficiently collected and the electromagnetic effect can be enhanced. As a result of this /ζ, the 1 market flux density in the above formula (1) is increased, and thereby a high sensitivity) W degree can be achieved. It should be noted that the Hall element chip 21 is first formed using a non-magnetic resin 28, and a magnetic resin 29 is further formed on both sides of the pole element chip 7 made of gallium arsenide. '21 is originally a non-magnetic material, and if it is sealed and molded with a resin with a general sound f social body, the magnetic flux will pass through the resin part instead of passing through the chip '21 'i', )S. Furthermore, according to the above embodiment, the thickness of the non-magnetic tree 11128 corresponds to the chip 21 and is formed so that it becomes thinner at the groin part, so that the magnetic resistance at this part is reduced. is the smallest. Therefore,
i1.] 11.
第4図は上記実施例によるホール素子と従来のものの出
力に正特性全対比させた特性図である。図示するように
、1薩、;泉Aで示したこの発明の実施例によるものの
方が、11′1線Bで示した従来のものよりも、同じイ
ft束密度1木でより大きな出力酸圧VHが碍られてい
ることがわかる。FIG. 4 is a characteristic diagram comparing the positive characteristics of the outputs of the Hall element according to the above embodiment and the conventional one. As shown in the figure, the embodiment of the present invention shown by Izumi A has a larger output acid at the same if flux density of 1 tree than the conventional one shown by 11'1 line B. It can be seen that the pressure VH is broken.
このようにこの発明による磁気レンジ−QJ:、感磁素
子を非磁性体461脂部材で平板状に封止1戎型し、さ
らにこの非磁性体樹脂部材ケそのデモ。斗両面から挾持
するように磁性体樹脂部材を成型するようにしたもので
8る。このため集磁効果が篩められてd石J盛度化が図
らノし、力゛リウムヒ累を用いた感磁素子の如き素子安
定性や信頼性は高いが高用力を得ることができないよう
なものに対しても容易に高感度化が達成でき、これによ
って素子安定性および信頼性と、惰感度特性とを同時に
満足する磁気センサが提IJ1.できる。+ ’、(:
li、感磁素子はガリウムヒ素以外の制別でイ11り成
aれるものを用いてもよい。As described above, in the magnetic range QJ according to the present invention, the magnetic sensing element was sealed in a flat plate shape with a non-magnetic resin material, and the non-magnetic resin material was further demonstrated. 8. A magnetic resin member is molded so as to be held between both sides of the dowel. For this reason, the magnetism collecting effect is sieved, and it is not possible to increase the density of magnetism, and although the stability and reliability of elements such as magneto-sensitive elements using a magneto-sensitive element using a magnetized aluminum alloy are high, it is difficult to obtain high usability. IJ1. proposes a magnetic sensor that can easily achieve high sensitivity even for objects, thereby satisfying element stability and reliability as well as inertia sensitivity characteristics at the same time. can. + ', (:
The magnetic sensing element may be made of materials other than gallium arsenide.
第1図はホール素子の出力′電圧測定回路ケ示す図、第
2図はこの発明の一実施例に、しるホール素子の斜視図
、第3図はそのIIJ?−1/I酉ン1、ζB4図は同
実施例のホール素子と従来のものの出力ll!I’性を
示す図である。
2)・・・ホール素子チッフ9.22・・・支時リート
ゝ、23・・・J?ンディングヮイヤ、24〜27・−
・外部リード、28・・・工、+5ギシ系樹脂(非磁性
体の11″!1脂)、29・・・樹脂(磁性体の樹脂)
。Fig. 1 is a diagram showing a circuit for measuring the output voltage of a Hall element, Fig. 2 is a perspective view of a Hall element according to an embodiment of the present invention, and Fig. 3 is a diagram showing its IIJ? -1/I 1, ζB4 diagram shows the output of the Hall element of the same embodiment and the conventional one! It is a figure showing I' nature. 2)...Hall element chip 9.22...time lead ゝ, 23...J? Endingwaya, 24-27・-
・External lead, 28...work, +5 cylindrical resin (non-magnetic material 11"!1 resin), 29...resin (magnetic material resin)
.
Claims (2)
型される非磁性体樹脂部材と、この非磁性体樹脂部材の
表裏両面を挾持するように成型される磁性体樹脂部材と
を具備したことを特徴とする磁気センサ。(1) A non-magnetic resin member molded into a flat plate shape to seal the magnetic sensing element, and a magnetic resin molded to sandwich both the front and back sides of the non-magnetic resin member. A magnetic sensor comprising a member.
応した部位の厚みが他の部位よりも薄く成型されている
特許請求の範囲第1項に記載の磁気センサ。(2) The magnetic sensor according to claim 1, wherein the non-magnetic resin member is molded to have a thickness thinner at a portion corresponding to the magnetic sensing element described in 01.1 than at other portions.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58187459A JPS6079281A (en) | 1983-10-06 | 1983-10-06 | Magnetic sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58187459A JPS6079281A (en) | 1983-10-06 | 1983-10-06 | Magnetic sensor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS6079281A true JPS6079281A (en) | 1985-05-07 |
Family
ID=16206443
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58187459A Pending JPS6079281A (en) | 1983-10-06 | 1983-10-06 | Magnetic sensor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6079281A (en) |
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4767989A (en) * | 1984-12-24 | 1988-08-30 | Alcatel N.V. | Mounting arrangement for magnetic field detector |
| JPS63313886A (en) * | 1987-06-17 | 1988-12-21 | Fujitsu Ltd | Superlattice |
| US5093617A (en) * | 1989-03-14 | 1992-03-03 | Mitsubishi Denki K.K. | Hall-effect sensor having integrally molded frame with printed conductor thereon |
| JP2002026419A (en) * | 2000-07-07 | 2002-01-25 | Sanken Electric Co Ltd | Magnetoelectric converter |
| US20180108617A1 (en) * | 2016-03-31 | 2018-04-19 | Tdk Corporation | Electronic circuit package using composite magnetic sealing material |
| US10269727B2 (en) * | 2016-03-31 | 2019-04-23 | Tdk Corporation | Composite magnetic sealing material and electronic circuit package using the same as mold material |
-
1983
- 1983-10-06 JP JP58187459A patent/JPS6079281A/en active Pending
Cited By (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4767989A (en) * | 1984-12-24 | 1988-08-30 | Alcatel N.V. | Mounting arrangement for magnetic field detector |
| JPS63313886A (en) * | 1987-06-17 | 1988-12-21 | Fujitsu Ltd | Superlattice |
| US5093617A (en) * | 1989-03-14 | 1992-03-03 | Mitsubishi Denki K.K. | Hall-effect sensor having integrally molded frame with printed conductor thereon |
| JP2002026419A (en) * | 2000-07-07 | 2002-01-25 | Sanken Electric Co Ltd | Magnetoelectric converter |
| US20180108617A1 (en) * | 2016-03-31 | 2018-04-19 | Tdk Corporation | Electronic circuit package using composite magnetic sealing material |
| US10256194B2 (en) * | 2016-03-31 | 2019-04-09 | Tdk Corporation | Electronic circuit package using composite magnetic sealing material |
| US10269727B2 (en) * | 2016-03-31 | 2019-04-23 | Tdk Corporation | Composite magnetic sealing material and electronic circuit package using the same as mold material |
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