JP2530115Y2 - YIG device - Google Patents

YIG device

Info

Publication number
JP2530115Y2
JP2530115Y2 JP40166190U JP40166190U JP2530115Y2 JP 2530115 Y2 JP2530115 Y2 JP 2530115Y2 JP 40166190 U JP40166190 U JP 40166190U JP 40166190 U JP40166190 U JP 40166190U JP 2530115 Y2 JP2530115 Y2 JP 2530115Y2
Authority
JP
Japan
Prior art keywords
magnetic core
shaped magnetic
yig
central axis
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.)
Expired - Lifetime
Application number
JP40166190U
Other languages
Japanese (ja)
Other versions
JPH0491402U (en
Inventor
隆 渡部
岳昭 森山
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.)
Advantest Corp
Original Assignee
Advantest 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 Advantest Corp filed Critical Advantest Corp
Priority to JP40166190U priority Critical patent/JP2530115Y2/en
Publication of JPH0491402U publication Critical patent/JPH0491402U/ja
Application granted granted Critical
Publication of JP2530115Y2 publication Critical patent/JP2530115Y2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Description

【考案の詳細な説明】[Detailed description of the invention]

【0001】[0001]

【産業上の利用分野】この考案は中心軸を有するつぼ形
磁気コアの開放面が板状磁気コアで蓋され、上記中心軸
の端面と板状磁気コアとの間にYIG素子が配され、中
心軸に巻回されたコイルに電流を流してYIG素子に磁
界を印加し、そのYIG素子を共鳴発振させ、発振回路
の共振器やろ波器に用いられるYIGデバイスに関す
る。
In the present invention, the open surface of a pot-shaped magnetic core having a central axis is covered with a plate-shaped magnetic core, and a YIG element is arranged between the end surface of the central axis and the plate-shaped magnetic core. The present invention relates to a YIG device used for a resonator or a filter of an oscillation circuit, by applying a current to a coil wound around a central axis to apply a magnetic field to a YIG element to cause the YIG element to resonate and oscillate.

【0002】[0002]

【従来の技術】図2に従来のYIGデバイスを示す。つ
ぼ形磁気コア11内の軸心位置に中心軸12が一体に形
成され、つぼ形磁気コア11の開放面は板状磁気コア1
3で蓋されている。中心軸12の端面と板状磁気コア1
3との間にYIG素子14が配される。つまりYIG素
子14は板状磁気コア13の内面に平行な支持棒15の
一端部に取付けられ、支持棒15の他端部は固定具16
で板状磁気コア13の内面に固定される。板状磁気コア
13の内面に混成集積回路基板17が固定される。
2. Description of the Related Art FIG. 2 shows a conventional YIG device. A central axis 12 is integrally formed at an axial center position in the pot-shaped magnetic core 11, and the open surface of the pot-shaped magnetic core 11 is
Covered with 3. End face of central shaft 12 and plate-shaped magnetic core 1
3, a YIG element 14 is arranged. That is, the YIG element 14 is attached to one end of a support rod 15 parallel to the inner surface of the plate-shaped magnetic core 13, and the other end of the support rod 15 is
Is fixed to the inner surface of the plate-shaped magnetic core 13. A hybrid integrated circuit board 17 is fixed to the inner surface of the plate-shaped magnetic core 13.

【0003】基板17に、YIG素子14が中心部に位
置するように半円形の結合リング18が取付けられ、結
合リング18は基板17上に形成された、図に示してい
ないが、共鳴したYIG素子14を共振器とする発振回
路と接続され、その発振出力を増幅する増幅器も基板1
7に形成されている。中心軸12にコイル19が巻回さ
れ、コイル19に電流を流してYIG素子14に磁界を
印加することができるようにされている。この磁界印加
によりYIG素子14が共鳴発振し、共振器として作用
させることができる。発振器として用いる場合、その発
振出力は、板状磁気コア13に取付けられた同軸出力端
子(コネクタ)21を通じて外部へ導出される。
[0003] A semi-circular coupling ring 18 is mounted on the substrate 17 so that the YIG element 14 is located at the center, and the coupling ring 18 is formed on the substrate 17. An amplifier connected to an oscillation circuit having the element 14 as a resonator and amplifying the oscillation output is also provided on the substrate 1.
7 is formed. A coil 19 is wound around the central axis 12 so that a current can flow through the coil 19 to apply a magnetic field to the YIG element 14. The application of the magnetic field causes the YIG element 14 to oscillate resonantly and function as a resonator. When used as an oscillator, its oscillation output is led out through a coaxial output terminal (connector) 21 attached to the plate-shaped magnetic core 13.

【0004】[0004]

【考案が解決しようとする課題】従来においては、つぼ
形磁気コア11として45ニッケル合金(Ni が45重
量%,残部がFe ,いわゆるPB)が用いられる。この
45ニッケル合金は溶融して形に入れて作る、つまり鋳
造(キャスティング)により、つぼ形磁気コア11を作
った場合は、磁界−電流特性の直線性が悪く、ヒステリ
シスが大きい。このため、YIG素子に印加する磁界の
強さに発振周波数が対応しているから、制御電流に対す
る発振周波数の直線性が悪く、かつ制御電流を増加した
時と、減少した時とで同一の大きさの制御電流でも発振
周波数が可なり異なったものとなる。このため、鋳造品
のつぼ形磁気コアは安価に作れるが実用化されていな
い。
Conventionally, a 45-nickel alloy (45% by weight of Ni, the balance being Fe, so-called PB) is used as the pot-shaped magnetic core 11. When this 45 nickel alloy is melted and formed into a shape, that is, when the crucible-shaped magnetic core 11 is formed by casting, the linearity of the magnetic field-current characteristic is poor and the hysteresis is large. Therefore, since the oscillation frequency corresponds to the strength of the magnetic field applied to the YIG element, the linearity of the oscillation frequency with respect to the control current is poor, and the same magnitude is obtained when the control current is increased and when the control current is decreased. Even with such a control current, the oscillation frequency is considerably different. For this reason, a pot-shaped magnetic core of a cast product can be manufactured at low cost, but has not been put to practical use.

【0005】つまり、従来では45ニッケル合金の円柱
状の鍛造品を切削加工して、中心軸12を有するつぼ形
磁気コア11を作ったものが用いられていた。この鍛造
品の切削加工により得られたものは鋳造により作ったも
のよりも、磁界−電流特性の直線性や、ヒステリシスが
1.3〜1.5倍近く良い。しかし、切削加工をするため加
工費が著しく高く、つぼ形磁気コアの内部の空間部分の
原材料が無駄になり、この点からも高価なものとなる欠
点があった。
In other words, conventionally, a pot-shaped magnetic core 11 having a center axis 12 is formed by cutting a forged product of a 45 nickel alloy column. The product obtained by cutting this forged product has better linearity and hysteresis of magnetic field-current characteristics than the product made by casting.
1.3 to 1.5 times better. However, the machining cost is extremely high due to the cutting process, and the raw material in the space inside the crucible-shaped magnetic core is wasted.

【0006】[0006]

【課題を解決するための手段】この考案によれば、中心
軸を有するつぼ形磁気コアはセンダストの鋳造品からな
る。
According to the invention, the crucible-shaped magnetic core having a central axis comprises a sendust casting.

【0007】[0007]

【実施例】図1にこの考案の実施例を示し、図2と対応
する部分に同一符号を付けてある。この考案では中心軸
12を有するつぼ形磁気コア11はセンダストの鋳造品
で構成されている。板状磁気コア13は45ニッケル合
金を切削加工して作ったものが用いられる。
FIG. 1 shows an embodiment of the present invention, in which parts corresponding to those in FIG. 2 are denoted by the same reference numerals. In the present invention, the pot-shaped magnetic core 11 having the central axis 12 is formed of a sendust casting. The plate-shaped magnetic core 13 is formed by cutting a 45 nickel alloy.

【0008】[0008]

【考案の効果】このように、この考案では中心軸を有す
るづぼ形磁気コアがセンダストの鋳造品で構成されてい
るため、センダストは磁気−電流特性の直線性がよく、
飽和レベルが高く、ヒステリシスが小さいから従来の4
5ニッケル合金の切削加工品と比べても、制御電流に対
する発振周波数の直線性や、制御電流を増加した時と減
少した時の同一制御電流に対する発振周波数ずれなど全
体的に特性が20〜30%向上した。しかも材料が安
く、かつ鋳造品であるため、安価に作ることができる。
As described above, in the present invention, since the wedge-shaped magnetic core having the central axis is formed of a Sendust casting, Sendust has good linearity in magnetic-current characteristics.
Since the saturation level is high and the hysteresis is small,
5 Compared to a 5 nickel alloy machined product, overall characteristics such as the linearity of the oscillation frequency with respect to the control current and the oscillation frequency deviation with respect to the same control current when the control current is increased and decreased are 20 to 30%. Improved. Moreover, since the material is inexpensive and a cast product, it can be manufactured at low cost.

【0009】前述したように、板状磁気コア13として
45ニッケル合金の切削加工品を用いる場合は、つぼ形
磁気コア11の開放端面と板状磁気コア13との接触を
良好に行わせることができる。
As described above, when a 45-nickel alloy cut product is used as the plate-shaped magnetic core 13, the open end surface of the pot-shaped magnetic core 11 and the plate-shaped magnetic core 13 can be brought into good contact. it can.

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

【図1】この考案の実施例を示す断面図。FIG. 1 is a sectional view showing an embodiment of the present invention.

【図2】従来のYIGデバイスを示す断面図。FIG. 2 is a sectional view showing a conventional YIG device.

Claims (1)

(57)【実用新案登録請求の範囲】(57) [Scope of request for utility model registration] 【請求項1】 中心軸を有するつぼ形磁気コアの開放面
が板状磁気コアで蓋され、上記中心軸の端面と上記板状
磁気コアとの間にYIG素子が配され、上記中心軸に巻
回されたコイルに電流を流して上記YIG素子に磁界を
印加するYIGデバイスにおいて、上記つぼ形磁気コア
はセンダストの鋳造品からなることを特徴とするYIG
デバイス。
An open surface of a pot-shaped magnetic core having a central axis is covered with a plate-shaped magnetic core, a YIG element is disposed between an end surface of the central axis and the plate-shaped magnetic core, and a YIG element is provided on the central axis. A YIG device for applying a magnetic field to the YIG element by applying a current to a wound coil, wherein the pot-shaped magnetic core is formed of a sendust casting.
device.
JP40166190U 1990-12-25 1990-12-25 YIG device Expired - Lifetime JP2530115Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP40166190U JP2530115Y2 (en) 1990-12-25 1990-12-25 YIG device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP40166190U JP2530115Y2 (en) 1990-12-25 1990-12-25 YIG device

Publications (2)

Publication Number Publication Date
JPH0491402U JPH0491402U (en) 1992-08-10
JP2530115Y2 true JP2530115Y2 (en) 1997-03-26

Family

ID=31879711

Family Applications (1)

Application Number Title Priority Date Filing Date
JP40166190U Expired - Lifetime JP2530115Y2 (en) 1990-12-25 1990-12-25 YIG device

Country Status (1)

Country Link
JP (1) JP2530115Y2 (en)

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
電子通信ハンドブック(昭和54年、オーム社)、P.365

Also Published As

Publication number Publication date
JPH0491402U (en) 1992-08-10

Similar Documents

Publication Publication Date Title
US4639624A (en) Torque motor having a coil with finite turning range
JP2530115Y2 (en) YIG device
JPS62202530U (en)
JPS5829673Y2 (en) electromagnetic speaker
JPS5936479B2 (en) Electromagnetic acoustic transducer
JPS5844719Y2 (en) Electromagnetic acoustic transducer
JPH0373099U (en)
JP2532330Y2 (en) YIG device
JPH0140170Y2 (en)
JPS6320165Y2 (en)
US4337449A (en) Magnetic transducer with a movable magnet
JPH0132325Y2 (en)
JPS6325820Y2 (en)
JPS6440248U (en)
JPS602632Y2 (en) Buzzer
JPS6123911Y2 (en)
JPH0818309A (en) Exciter for yig device
JPS602634Y2 (en) Magnetic electronic buzzer
JPH0233413U (en)
JPH082803Y2 (en) Magnetic head
JPS6145739Y2 (en)
JPH0522985Y2 (en)
JPH048967U (en)
JPH07249905A (en) Magnetic circuit for yig device and its manufacture
JPH04251902A (en) Magnetic core

Legal Events

Date Code Title Description
A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 19960910