JP2985469B2 - Pulse magnetic field generator - Google Patents

Pulse magnetic field generator

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Publication number
JP2985469B2
JP2985469B2 JP4016276A JP1627692A JP2985469B2 JP 2985469 B2 JP2985469 B2 JP 2985469B2 JP 4016276 A JP4016276 A JP 4016276A JP 1627692 A JP1627692 A JP 1627692A JP 2985469 B2 JP2985469 B2 JP 2985469B2
Authority
JP
Japan
Prior art keywords
magnetic field
pulse
yoke
field generator
magnetic
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
JP4016276A
Other languages
Japanese (ja)
Other versions
JPH05217742A (en
Inventor
千尋 築島
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP4016276A priority Critical patent/JP2985469B2/en
Publication of JPH05217742A publication Critical patent/JPH05217742A/en
Application granted granted Critical
Publication of JP2985469B2 publication Critical patent/JP2985469B2/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】この発明は、少ないパルス電流に
よって強力な磁界を発生することができるパルス磁場発
生装置に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a pulse magnetic field generator capable of generating a strong magnetic field with a small pulse current.

【0002】[0002]

【従来の技術】図4は例えば「昭和48年度・文部省科
学研究費総合研究A−834021・SOR−RING
REPORT・NO3」に示された従来のパルス電磁
石の構成を示す斜視図、図5は図4におけるパルス電磁
石の駆動電源回路を示す回路図である。図において、1
は断面コ字状に形成されたコア、2はこのコア1の空隙
部に装着されるコイルであり、これらでパルス電磁石3
を構成している。4はパルス電源、5はこのパルス電源
4とパルス電磁石3のコイル2間に介在する放電スイッ
チである。
2. Description of the Related Art FIG. 4 shows, for example, "Study 1975, Research Grant-in-Aid for Scientific Research A-834021, SOR-RING"
REPORT.NO3 "is a perspective view showing the configuration of the conventional pulse electromagnet shown in FIG. 5, and FIG. 5 is a circuit diagram showing a drive power supply circuit for the pulse electromagnet in FIG. In the figure, 1
Is a core formed in a U-shaped cross section, and 2 is a coil mounted in a gap of the core 1, and these are used as pulse electromagnets 3.
Is composed. Reference numeral 4 denotes a pulse power supply, and 5 denotes a discharge switch interposed between the pulse power supply 4 and the coil 2 of the pulse electromagnet 3.

【0003】次に上記のように構成された従来装置の動
作について説明する。まず、放電スイッチ5を投入する
と、パルス電源4よりパルス電磁石3のコイル2にパル
ス電流が供給されヨーク1の空隙にはパルス磁界が発生
し供試磁場として種々の目的に使用される。今、このヨ
ーク1を形成する物質の透磁率が空隙内の透磁率と比較
して十分に大きい場合、空隙内に発生する磁束の磁束密
度Bはパルス電流をI、空隙の幅をd、空隙内の透磁率
をμとすると以下に示す式(1)で得られる。 B=μI/d (1)
[0003] Next, the operation of the conventional apparatus configured as described above will be described. First, when the discharge switch 5 is turned on, a pulse current is supplied from the pulse power supply 4 to the coil 2 of the pulse electromagnet 3, and a pulse magnetic field is generated in the gap of the yoke 1 and used as a test magnetic field for various purposes. Now, if the magnetic permeability of the material forming the yoke 1 is sufficiently large compared to the magnetic permeability in the air gap, the magnetic flux density B of the magnetic flux generated in the air gap is I, the pulse current is I, the air gap width is d, and the air gap is d. Is given by the following equation (1), where μ is the magnetic permeability. B = μI / d (1)

【0004】[0004]

【発明が解決しようとする課題】従来のパルス磁場発生
装置は以上のように構成され、供試磁場内の磁界の強さ
は式(1)にて得られる磁束密度Bの大きさで決定され
るので、磁界の強さを上げるためには、空隙の幅dを狭
くするか、又はコイル2に流すパルス電流を大きくしな
ければならないが、空隙の幅dを狭くすると磁場領域が
限定されて適用範囲が狭くなり、又、パルス電流を大き
くするためには大容量のパルス電源4が必要になる等の
問題点があった。
The conventional pulse magnetic field generator is constructed as described above, and the strength of the magnetic field in the test magnetic field is determined by the magnitude of the magnetic flux density B obtained by the equation (1). Therefore, in order to increase the strength of the magnetic field, the width d of the air gap must be reduced or the pulse current flowing through the coil 2 must be increased. However, when the width d of the air gap is reduced, the magnetic field region is limited. There have been problems such as a narrower application range and a need for a large-capacity pulse power supply 4 to increase the pulse current.

【0005】この発明は上記のような問題点を解消する
ためになされたもので、小さいパルス電流で強磁界を得
ることが可能なパルス磁場発生装置を提供することを目
的とするのものである。
The present invention has been made to solve the above problems, and has as its object to provide a pulse magnetic field generator capable of obtaining a strong magnetic field with a small pulse current. .

【0006】[0006]

【課題を解決するための手段】この発明に係るパルス磁
場発生装置は、供試磁場に磁界をかける磁界発生装置
と、飽和特性を有する強磁性体でなり且つ磁路の一部が
供試磁場に並設されるとともに磁路の一部に磁界発生装
置による磁束が流れるのを許容するヨークと、このヨー
クにパルス磁界をかけヨークを飽和させることにより磁
路の一部を流れる磁界発生装置による磁束を供試磁場側
を流れるようになすパルス電源とを備えたものである。
A pulse magnetic field generator according to the present invention includes a magnetic field generator for applying a magnetic field to a test magnetic field, a ferromagnetic material having a saturation characteristic, and a part of a magnetic path of the test magnetic field. And a yoke that allows the magnetic flux from the magnetic field generator to flow through a part of the magnetic path and a magnetic field generator that flows through a part of the magnetic path by applying a pulse magnetic field to the yoke to saturate the yoke A pulse power supply for causing a magnetic flux to flow on the test magnetic field side.

【0007】[0007]

【作用】この発明におけるパルス磁場発生装置のパルス
電源は、常時はヨークの磁路の一部を流れている磁界発
生装置による磁束を、ヨークにパルス電流を流して飽和
させることにより供試磁場側に流す。
The pulse power supply of the pulse magnetic field generator according to the present invention uses a magnetic field generated by the magnetic field generator, which normally flows through a part of the magnetic path of the yoke, to saturate the yoke by applying a pulse current to the yoke. Pour into

【0008】[0008]

【実施例】【Example】

実施例1.以下、この発明の実施例を図について説明す
る。図1はこの発明の実施例1におけるパルス磁場発生
装置の概略構成を示す図である。図において、6はヨー
ク6aと、このヨーク6aに巻回されるコイル6bと、
このコイル6bに電流Iを供給する磁界発生用電源6c
とでなる外部磁界発生装置、7は種々の目的に供試され
る供試磁場、8は磁路の一部8aがこの供試磁場7に並
設されるヨーク、9はこのヨーク8に巻回されるコイ
ル、10はこのコイル9にパルス電流I′を供給するパ
ルス電源、11はコイル9および電源10を接続する回
路をON、OFFする放電スイッチである。
Embodiment 1 FIG. Hereinafter, an embodiment of the present invention will be described with reference to the drawings. FIG. 1 is a diagram showing a schematic configuration of a pulse magnetic field generator according to Embodiment 1 of the present invention. In the figure, 6 is a yoke 6a, a coil 6b wound around the yoke 6a,
Power supply 6c for generating magnetic field for supplying current I to coil 6b
An external magnetic field generator 7; a test magnetic field to be tested for various purposes; 8, a yoke in which a portion 8a of a magnetic path is arranged in parallel with the test magnetic field 7; The coil 10 to be turned is a pulse power supply for supplying a pulse current I 'to the coil 9, and 11 is a discharge switch for turning on and off a circuit connecting the coil 9 and the power supply 10.

【0009】次に上記のように構成されたこの発明の実
施例1におけるパルス磁場発生装置の動作について説明
する。まず、図1−(A)に示すように、予め磁界発生
用電源6cによってコイル6bに電流Iを流し、ヨーク
6aを介してヨーク8の磁路の一部8aが飽和する近く
の磁界を発生させる。この時、磁路の一部8aの近傍、
すなわち供試磁場7内の点Pでは、外部磁界発生装置6
による磁束は透磁率の高いヨーク8の磁路の一部8aを
通って流れるため発生磁界は小さくなっている。次に、
図1−(B)に示すように、放電スイッチ11をONし
てコイル9にパルス電流I′を流して、ヨーク8中に磁
路の一部8aを流れる外部磁界発生装置6による磁束と
同方向に流れる磁束を発生させヨーク8を飽和させる。
ヨーク8が飽和すると透磁率が低下するため、今までヨ
ーク8の磁路の一部8aを通っていた磁束は点P、すな
わち供試磁場7側を流れるようになり、この位置にパル
ス状の磁界を発生させることができる。
Next, the operation of the pulse magnetic field generator according to the first embodiment of the present invention will be described. First, as shown in FIG. 1- (A), a current I is applied to the coil 6b in advance by the magnetic field generating power supply 6c, and a magnetic field near the saturation of a part 8a of the magnetic path of the yoke 8 is generated via the yoke 6a. Let it. At this time, near the part 8a of the magnetic path,
That is, at the point P in the test magnetic field 7, the external magnetic field generator 6
Generates a small magnetic field because it flows through a portion 8a of the magnetic path of the yoke 8 having high magnetic permeability. next,
As shown in FIG. 1- (B), the discharge switch 11 is turned on, a pulse current I ′ flows through the coil 9, and the same as the magnetic flux generated by the external magnetic field generator 6 flowing through the magnetic path 8 a in the yoke 8. A magnetic flux flowing in the direction is generated to saturate the yoke 8.
When the yoke 8 saturates, the magnetic permeability decreases, so that the magnetic flux that has passed through a portion 8a of the magnetic path of the yoke 8 now flows at the point P, that is, the test magnetic field 7 side. A magnetic field can be generated.

【0010】このようにして供試磁場7中に発生される
パルス状の磁界は、外部磁界発生装置6のヨーク6aの
空隙の幅およびヨーク6a内の磁束の通過長さに依存す
る。したがって、パルス電源10によって供給しなけれ
ばならないパルス電流は、ヨーク8を飽和できる最低の
電流で良いことになる。このときヨーク8内の透磁率を
μ′、ヨーク8が飽和する磁束密度をB′、ヨーク8内
の磁束の通る長さをLとすると、必要なパルス電流I′
は以下に示す式(2)で得られる。 I′=B′L/μ′ (2) ここで、従来の方式で必要なパルス電流Iは式(1)よ
り以下に示す式(3)となる。 I=Bd/μ (3) 今、上記式(2)および式(3)より、B〜B′の磁場
を発生する場合、L〜d、μ<<μ′であるので、上記
実施例1においては極めて小さいパルス電流I′で所望
の磁場が得られることは明らかである。
The pulsed magnetic field generated in the test magnetic field 7 depends on the width of the gap of the yoke 6a of the external magnetic field generator 6 and the length of the magnetic flux passing through the yoke 6a. Therefore, the pulse current that has to be supplied by the pulse power supply 10 is a minimum current that can saturate the yoke 8. At this time, assuming that the magnetic permeability in the yoke 8 is μ ′, the magnetic flux density at which the yoke 8 saturates is B ′, and the length of the magnetic flux in the yoke 8 is L, the necessary pulse current I ′
Is obtained by the following equation (2). I ′ = B′L / μ ′ (2) Here, the pulse current I required in the conventional method is given by the following equation (3) from the equation (1). I = Bd / μ (3) Now, from the above equations (2) and (3), when a magnetic field of B to B ′ is generated, L to d and μ << μ ′. It is clear that the desired magnetic field can be obtained with an extremely small pulse current I '.

【0011】実施例2.図2はこの発明の実施例2にお
けるパルス磁場発生装置を示す斜視図である。図から明
らかなように、装置自身は図1に示す実施例1のものと
同様であるが、供試磁場7を荷電粒子ビーム装置の電子
ビーム12の偏向磁場として適用したものである。
Embodiment 2 FIG. FIG. 2 is a perspective view showing a pulse magnetic field generator according to Embodiment 2 of the present invention. As is clear from the figure, the device itself is the same as that of the first embodiment shown in FIG. 1, but the test magnetic field 7 is applied as a deflection magnetic field of the electron beam 12 of the charged particle beam device.

【0012】実施例3.図3はこの発明の実施例3にお
けるパルス磁場発生装置を示す斜視図である。図におい
て、13はシンクロトロンまたは蓄積リングの偏向電磁
石であり、上記各実施例と同様な部分は同一符号を付し
て説明を省略する。前述の実施例2は実施例1における
磁場発生装置の供試磁場7を荷電粒子ビーム装置のビー
ム偏向磁場に適用したものであるのに対して、この実施
例3は実施例1における磁場発生装置の外部磁界発生装
置6を、シンクロトロンまたは蓄積リングの偏向電磁石
13で兼用したものであり、上記各実施例同様の効果を
奏することは勿論のこと、外部磁界発生装置6を省略し
たことによる装置の簡単化ならびに小型化を図ることも
可能になる。
Embodiment 3 FIG. FIG. 3 is a perspective view showing a pulse magnetic field generator according to Embodiment 3 of the present invention. In the figure, reference numeral 13 denotes a synchrotron or a storage ring deflection electromagnet, and the same parts as those in the above-described embodiments are denoted by the same reference numerals and description thereof is omitted. In the second embodiment described above, the test magnetic field 7 of the magnetic field generator of the first embodiment is applied to the beam deflection magnetic field of the charged particle beam device, whereas in the third embodiment, the magnetic field generator of the first embodiment is applied. The external magnetic field generator 6 is also used as a synchrotron or a storage ring deflecting electromagnet 13. The same effects as those of the above embodiments can be obtained, and the external magnetic field generator 6 can be omitted. Simplification and downsizing can be achieved.

【0013】[0013]

【発明の効果】以上のように、この発明によれば供試磁
場に磁界をかける磁界発生装置と、飽和特性を有する強
磁性体でなり且つ磁路の一部が供試磁場に並設されると
ともに磁路の一部に磁界発生装置による磁束が流れるの
を許容するヨークと、このヨークにパルス磁界をかけヨ
ークを飽和させることにより磁路の一部を流れる磁界発
生装置による磁束を供試磁場側を流れるようになすパル
ス電源とを備えたので小さいパルス電流で強磁界を得る
ことが可能なパルス磁場発生装置を提供することができ
る。
As described above, according to the present invention, a magnetic field generator for applying a magnetic field to a test magnetic field and a ferromagnetic material having a saturation characteristic and a part of a magnetic path are provided in parallel with the test magnetic field. A yoke that allows the magnetic flux generated by the magnetic field generator to flow through a part of the magnetic path and a magnetic field generated by the magnetic field generator that flows through a part of the magnetic path by applying a pulse magnetic field to the yoke to saturate the yoke Since a pulse power supply is provided to flow on the magnetic field side, a pulse magnetic field generator capable of obtaining a strong magnetic field with a small pulse current can be provided.

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

【図1】この発明の実施例1におけるパルス磁場発生装
置を示すもので、(A)は電源投入前、(B)は電源投
入後の状態をそれぞれ示す斜視図である。
FIG. 1 is a perspective view showing a pulse magnetic field generating device according to a first embodiment of the present invention, in which (A) shows a state before power is turned on, and (B) shows a state after power is turned on.

【図2】この発明の実施例2におけるパルス磁場発生装
置を示す斜視図である。
FIG. 2 is a perspective view showing a pulse magnetic field generator according to Embodiment 2 of the present invention.

【図3】この発明の実施例3におけるパルス磁場発生装
置を示す斜視図である。
FIG. 3 is a perspective view showing a pulse magnetic field generator according to Embodiment 3 of the present invention.

【図4】従来のパルス電磁石の構成を示す斜視図であ
る。
FIG. 4 is a perspective view showing a configuration of a conventional pulse electromagnet.

【図5】図4におけるパルス電磁石の駆動電源回路を示
す回路図である。
FIG. 5 is a circuit diagram showing a drive power supply circuit for the pulse electromagnet in FIG. 4;

【符号の説明】[Explanation of symbols]

6 磁界発生装置 7 供試磁場 8 ヨーク 8a 磁路の一部 10 パルス電源 11 放電スイッチ 13 偏向電磁石 Reference Signs List 6 magnetic field generator 7 test magnetic field 8 yoke 8a part of magnetic path 10 pulse power supply 11 discharge switch 13 deflection electromagnet

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 供試磁場に磁界をかける磁界発生装置
と、飽和特性を有する強磁性体でなり且つ磁路の一部が
上記供試磁場に並設されるとともに上記磁路の一部に上
記磁界発生装置による磁束が流れるのを許容するヨーク
と、上記ヨークにパルス磁界をかけ上記ヨークを飽和さ
せることにより上記磁路の一部を流れる上記磁界発生装
置による磁束を上記供試磁場側を流れるようになすパル
ス電源とを備えたことを特徴とするパルス磁場発生装
置。
A magnetic field generator for applying a magnetic field to a test magnetic field, a ferromagnetic material having a saturation characteristic, and a part of a magnetic path is juxtaposed to the test magnetic field and a part of the magnetic path is provided. A yoke that allows the magnetic flux generated by the magnetic field generator to flow, and a magnetic field generated by the magnetic field generator that flows through a part of the magnetic path by applying a pulse magnetic field to the yoke to saturate the yoke. A pulsed magnetic field generator, comprising: a pulsed power supply for flowing.
【請求項2】 ヨークを円形加速器の偏向電磁石の空隙
内に配設し上記偏向電磁石を磁界発生装置として兼用し
たことを特徴とする請求項1記載のパルス磁場発生装
置。
2. The pulse magnetic field generator according to claim 1, wherein the yoke is disposed in a gap between the deflection electromagnets of the circular accelerator, and the deflection electromagnets are used also as a magnetic field generator.
JP4016276A 1992-01-31 1992-01-31 Pulse magnetic field generator Expired - Fee Related JP2985469B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4016276A JP2985469B2 (en) 1992-01-31 1992-01-31 Pulse magnetic field generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4016276A JP2985469B2 (en) 1992-01-31 1992-01-31 Pulse magnetic field generator

Publications (2)

Publication Number Publication Date
JPH05217742A JPH05217742A (en) 1993-08-27
JP2985469B2 true JP2985469B2 (en) 1999-11-29

Family

ID=11912029

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4016276A Expired - Fee Related JP2985469B2 (en) 1992-01-31 1992-01-31 Pulse magnetic field generator

Country Status (1)

Country Link
JP (1) JP2985469B2 (en)

Also Published As

Publication number Publication date
JPH05217742A (en) 1993-08-27

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