JPH0260035A - Permanent magnet for electron lens - Google Patents
Permanent magnet for electron lensInfo
- Publication number
- JPH0260035A JPH0260035A JP21035188A JP21035188A JPH0260035A JP H0260035 A JPH0260035 A JP H0260035A JP 21035188 A JP21035188 A JP 21035188A JP 21035188 A JP21035188 A JP 21035188A JP H0260035 A JPH0260035 A JP H0260035A
- Authority
- JP
- Japan
- Prior art keywords
- permanent magnet
- ring
- yoke
- shaped permanent
- permanent magnets
- 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
- 230000005291 magnetic effect Effects 0.000 claims abstract description 35
- 229910045601 alloy Inorganic materials 0.000 claims abstract description 6
- 239000000956 alloy Substances 0.000 claims abstract description 6
- 238000009826 distribution Methods 0.000 claims abstract description 6
- 230000004907 flux Effects 0.000 claims description 9
- 238000010894 electron beam technology Methods 0.000 claims description 6
- 239000003302 ferromagnetic material Substances 0.000 claims description 3
- 230000005294 ferromagnetic effect Effects 0.000 claims 1
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 abstract description 11
- 239000000463 material Substances 0.000 abstract description 5
- 238000010276 construction Methods 0.000 abstract 1
- 229910052710 silicon Inorganic materials 0.000 abstract 1
- 239000010703 silicon Substances 0.000 abstract 1
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 5
- 238000000605 extraction Methods 0.000 description 5
- 238000007796 conventional method Methods 0.000 description 4
- 238000000034 method Methods 0.000 description 4
- 229910052799 carbon Inorganic materials 0.000 description 3
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 2
- 229910000828 alnico Inorganic materials 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 229910052742 iron Inorganic materials 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 229910001209 Low-carbon steel Inorganic materials 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、例えばプロジェクタ−用プラン管の電子ビー
ム制御用に、使われる電子レンズ用永久磁石の改良に関
する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an improvement in a permanent magnet for an electron lens used, for example, for controlling an electron beam of a plan tube for a projector.
従来、この種の装置例として特開昭61−211940
号[以下、これを「引例例」という]がある。Conventionally, as an example of this type of device, Japanese Patent Application Laid-Open No. 61-211940
No. [hereinafter referred to as ``example citation''].
この従来例は、リングの中心軸方向であるZ軸方向に別
個に着磁され、同一磁極方向に連結された少なくとも2
個のリング状永久磁石から成り、これらリング状永久磁
石が2軸上の磁束分布の半値幅がそのリング状永久磁石
の内径の80〜200%の値を有するとともに、それら
リング状永久磁石の各両端面にはいずれも磁極片を備え
る電子レンズ用永久磁石である。In this conventional example, at least two magnets are separately magnetized in the Z-axis direction, which is the central axis direction of the ring, and are connected in the same magnetic pole direction.
These ring-shaped permanent magnets have a half-value width of magnetic flux distribution on two axes that is 80 to 200% of the inner diameter of the ring-shaped permanent magnet, and each of these ring-shaped permanent magnets has a This is a permanent magnet for an electronic lens that has magnetic pole pieces on both end faces.
しかし従来例は、リング状永久磁石がZ軸上の磁束分布
の半値幅がある程度にしようとすると、リング状永久磁
石のZ軸方向の長さ(厚み)を相当に長くしなければな
らず、そのためリング状永久磁石の製造も困難で、かつ
高価になる。However, in the conventional example, if the ring-shaped permanent magnet is to have a certain half-value width of the magnetic flux distribution on the Z-axis, the length (thickness) of the ring-shaped permanent magnet in the Z-axis direction must be made considerably long. Therefore, it is difficult and expensive to manufacture ring-shaped permanent magnets.
そこで、本出願人は先にこれを解決する特願昭63−1
02928号[以下、これを「先行例」という。]を提
案した。Therefore, the present applicant first filed a patent application filed in 1986-1 to solve this problem.
No. 02928 [hereinafter referred to as "precedent example"]. ] was proposed.
第3図はこの先行例の説明図で、第3図(a)はその側
断面図、第3図(b)は平面図を表す。FIG. 3 is an explanatory diagram of this prior example, with FIG. 3(a) showing its side sectional view and FIG. 3(b) showing its plan view.
リング状永久磁石1a、lbはZ軸方向つまり電子銃[
図示せず]から放射される電子ビーム8の進行方向に図
示のように着磁されかつ強磁性体からなる継鉄を両リン
グ状永久磁石1a、lb端面で挟み付けて圧接挿入して
おり、その両磁極端面には磁性体のリング状の磁極片2
a、2bが接着され、更にZ軸中心の磁束9に基づく磁
界の強さをコントロールするためのコイル5がボビン4
に巻かれてリング状永久磁石1a、lbの内部に装着さ
れている。The ring-shaped permanent magnets 1a and lb are aligned in the Z-axis direction, that is, in the electron gun [
A yoke made of a ferromagnetic material and magnetized as shown in the figure is inserted in the traveling direction of the electron beam 8 emitted from the ring-shaped permanent magnets 1a and lb by sandwiching them between the end faces of the ring-shaped permanent magnets 1a and lb. A ring-shaped magnetic pole piece 2 made of magnetic material is attached to the end faces of both magnetic poles.
a and 2b are glued together, and a coil 5 for controlling the strength of the magnetic field based on the magnetic flux 9 centered on the Z-axis is attached to the bobbin 4.
The magnets are wound around and mounted inside the ring-shaped permanent magnets 1a and lb.
当然、コイル5はリード線7で外部に連絡される。Naturally, the coil 5 is connected to the outside via a lead wire 7.
そのため、通常は磁極片2aあるいは2bの一方に取出
孔6を設ける必要がある。Therefore, it is usually necessary to provide an extraction hole 6 in one of the magnetic pole pieces 2a or 2b.
また、通常の磁極片又は継鉄は炭素量0. 3%以下程
度の軟鉄が使用される。Also, ordinary magnetic pole pieces or yoke have a carbon content of 0. Soft iron of about 3% or less is used.
しかるに、このようにリード線7を外部へ取出すための
取出孔6を磁極片2aに設けることは、その磁極片2a
の物理的条件を不均一とじ、ひいては磁束9に基づく磁
界の強さを乱すことになる。However, providing the extraction hole 6 for taking out the lead wire 7 to the outside in the magnetic pole piece 2a means that the magnetic pole piece 2a
This results in non-uniform physical conditions of the magnetic flux 9, which in turn disturbs the strength of the magnetic field based on the magnetic flux 9.
また、磁極片又は継鉄は炭素量0.3%以下程度の軟鉄
が使用されるためそのため、近辺に高周波磁界が発生す
る場合には、渦流損等による有害な昇熱が生起するよう
になる。In addition, since soft iron with a carbon content of about 0.3% or less is used for the magnetic pole piece or yoke, if a high-frequency magnetic field is generated nearby, harmful heat rise will occur due to eddy current loss, etc. .
ここにおいて本発明は、従来例・、先行例にみられるこ
れらの難点を克服した電子レンズ用永久磁石を提供する
ことを、その目的とする。SUMMARY OF THE INVENTION An object of the present invention is to provide a permanent magnet for an electronic lens that overcomes these difficulties seen in the conventional and precedent examples.
上記目的を達成するために、本発明は、例えばSt元素
を含有し電気固有抵抗が20マイクロオーム・センチメ
ートル以上に高められた成分でリード線を外部に取出す
ための溝が1〜2個所設けられたリング状継鉄を焼結材
から成る焼結体で作成し、そのリング状継鉄を両リング
状永久磁石端で挟み付けて電子レンズ用永久磁石を形成
する。In order to achieve the above object, the present invention is made of a component containing, for example, St element and having an increased electric resistivity of 20 micro ohm cm or more, and is provided with one or two grooves for taking out the lead wire to the outside. The ring-shaped yoke is made of a sintered body made of a sintered material, and the ring-shaped yoke is sandwiched between the ends of both ring-shaped permanent magnets to form a permanent magnet for an electron lens.
上記のように構成しているから、内蔵されているコイル
のリード線を外部に導出する場合に、磁極片にリード線
の取出孔を設けて磁界分布を乱すことがなく、かつ焼結
合金であるためにリング状の継鉄の端部に溝を開設する
ことは容易である。Because of the structure described above, when leading the lead wire of the built-in coil to the outside, there is no need to provide a lead wire extraction hole in the magnetic pole piece and disturb the magnetic field distribution, and the sintered alloy is used. Therefore, it is easy to create a groove at the end of a ring-shaped yoke.
また、焼結合金であるためSt元索等の添加成分によっ
て固有抵抗を増すことも容易である。Further, since it is a sintered alloy, it is easy to increase the specific resistance by adding components such as St base wire.
本発明の一実施例における形状を第1図に表す。 The shape of one embodiment of the present invention is shown in FIG.
第1図(a)は側面図、第1図(b)は一部を切り欠い
だ平面図である。FIG. 1(a) is a side view, and FIG. 1(b) is a partially cutaway plan view.
すべての図面において、同一符号は同一部材を示す。In all drawings, the same reference numerals indicate the same parts.
リング状永久磁石1a、lbは外径58φmm。The ring-shaped permanent magnets 1a and lb have an outer diameter of 58φmm.
内径48φmm、厚み8mmのアルニコ(A l n
i cO・8商標名)よりなる磁石で、その外側両端面
に各々外径56φam、内径33φmm、厚み3III
11のリング状の磁極片2a、2bを接合固着する。Alnico (Alnico) with inner diameter 48φmm and thickness 8mm
A magnet made of i cO・8 (trade name), with an outer diameter of 56φam, an inner diameter of 33φmm, and a thickness of 3III on both outer end surfaces.
Eleven ring-shaped magnetic pole pieces 2a and 2b are bonded and fixed.
耐熱性ボビン4に例えば0.18φ關の絶縁銅線を約5
30回巻いたコイル5を内蔵する。For example, attach about 5 insulated copper wires of 0.18φ to the heat-resistant bobbin 4.
It has a built-in coil 5 wound 30 times.
そして、リング状永久磁石1a、lbとほぼ同一の外径
と内径で厚み9報のリング状の焼結材から成る焼結体・
継鉄30の端面に幅2〜3m+s、深さ2IIImの溝
〔取出溝10〕を焼結体用成形金型によって開設する。Then, a sintered body made of a ring-shaped sintered material with approximately the same outer diameter and inner diameter as the ring-shaped permanent magnets 1a and lb and a thickness of 9.
A groove [removal groove 10] having a width of 2 to 3 m+s and a depth of 2 III m is opened in the end face of the yoke 30 using a mold for forming a sintered body.
その焼結体・継鉄30の成分は、例えば3.08%のS
t元素を含むFeベースの成分で、その電気固有抵抗率
は35マイクロオーム・センナメートルである。The composition of the sintered body/yoke 30 is, for example, 3.08% S.
It is a Fe-based component containing the element T and has an electrical resistivity of 35 microohm sennamometers.
このようにして作成した本発明に成る電子レンズ用永久
磁石[これを、r本発明の方法」と表すっと、
それと同一の外径と内径と厚みを持つ従来の例えば0,
25%のC元素を含む低炭素鋼で継鉄3を作成し〔ただ
し取出溝10は備えていない〕、コイル5のリード線7
を取出すためにリング状の磁極片2aあるいは2bの一
方に2,5φ關の取出孔6を穿孔した場合[これを「従
来の方法」と示す]と、
をそれぞれ電子ビーム8の中心軸より10關離れた箇所
での磁束9による磁界の強さのバラツキを次の表に示し
た。The permanent magnet for an electronic lens according to the present invention produced in this way [hereinafter referred to as "the method of the present invention"] is a permanent magnet for an electronic lens that has the same outer diameter, inner diameter, and thickness as the permanent magnet for an electronic lens according to the present invention.
The yoke 3 is made of low carbon steel containing 25% C element [however, it does not have the take-out groove 10], and the lead wire 7 of the coil 5 is made.
When a 2.5φ extraction hole 6 is bored in one of the ring-shaped magnetic pole pieces 2a or 2b in order to take out the electron beam (this is referred to as the "conventional method"), The following table shows the variation in the strength of the magnetic field due to the magnetic flux 9 at distant locations.
ここに、偏磁率とは[(最大値−最小値)/(最大値)
]X100をいう。Here, polarization is [(maximum value - minimum value) / (maximum value)
]X100.
このように、本発明は従来例・先行例に較べて、磁界の
バラツキが明らかに小さい。As described above, the present invention has clearly smaller variations in the magnetic field than the conventional and preceding examples.
つぎに、某社製の電子ビーム・プロジェクタ−[それを
「従来の方法」とする]と、本発明のそれとを同一条件
でセット通電し、ソケット側磁極片における表面温度を
熱電対によって測定した。Next, an electron beam projector manufactured by a certain company [this will be referred to as the "conventional method"] and that of the present invention were energized under the same conditions, and the surface temperature of the socket-side magnetic pole piece was measured with a thermocouple.
その結果は、第2図に21本発明の方法および22従来
の方法の特性曲線として表される。The results are represented in FIG. 2 as characteristic curves for 21 the method of the present invention and 22 the conventional method.
明らかに、本発明の方法による場合の温度上昇が少ない
。Clearly, the temperature rise is lower with the method of the invention.
かくして本発明は、リング状永久磁石並びにリング状の
継鉄に内蔵され円筒状ボビンに巻回されたコイルのリー
ド線を外部に取出すのに磁界分布を乱すことなく、かつ
継鉄における取出溝の開設も容易であり、継鉄が焼結合
金から成るので添加成分により電気固有抵抗を増加させ
渦流損に基づく昇熱を著しく抑制できるという、数多く
の格段の効果を奏する。Thus, the present invention enables the lead wires of the ring-shaped permanent magnet and the coil built in the ring-shaped yoke and wound around the cylindrical bobbin to be taken out to the outside without disturbing the magnetic field distribution, and without disturbing the extraction groove in the yoke. It is easy to install, and since the yoke is made of a sintered alloy, the added components can increase the electrical resistivity and significantly suppress heat rise due to eddy current loss.
第1図は本発明の一実施例の側面図、一部を切欠いた平
面図、第2図は本発明の方法と従来の方法の渦流損に基
づく昇熱比較図、第3図は先行例の説明図である。
la、lb・・・リング状永久磁石
2a、2b・・・リング状磁極片
3・・・継鉄[先行例]
30・・・強磁性体からなる継鉄[本発明]4・・・ボ
ビン
5・・・コイル
6・・・取出孔[先行例]
7・・・リード線
8・・・電子ビーム
9・・・磁束
10・・・取出溝[本発明〕。
出願人代理人 佐 藤 −雄
(α)
(b)
第1図
8存
間(分)−
第2図Figure 1 is a side view and partially cutaway plan view of an embodiment of the present invention, Figure 2 is a comparison diagram of heat rise based on eddy flow loss between the method of the present invention and the conventional method, and Figure 3 is a prior example. FIG. la, lb...Ring-shaped permanent magnets 2a, 2b...Ring-shaped magnetic pole pieces 3...Yoke [preceding example] 30...Yoke made of ferromagnetic material [present invention] 4...Bobbin 5... Coil 6... Take-out hole [preceding example] 7... Lead wire 8... Electron beam 9... Magnetic flux 10... Take-out groove [present invention]. Applicant's agent - Yu Sato (α) (b) Figure 1 8 duration (minutes) - Figure 2
Claims (1)
一磁極方向に連結された少なくとも2個のリング状永久
磁石内孔部を電子ビームが通過する電子レンズ用永久磁
石において、 隣接するリング状永久磁石相互間に、 それらリング状永久磁石とほぼ内径、外径を等しくしZ
軸方向の長さを任意とする強磁性体からなる継鉄を両リ
ング状永久磁石端面で挟み付けて圧接挿入し、 Z軸上の磁束密度分布の半値幅を高めるようにするとと
もに、 継鉄は、その継鉄とリング状永久磁石に内蔵するコイル
のリード線を取出す溝を1個以上設けた焼結合金で構成
する ことを特徴とする電子レンズ用永久磁石。 2、前記電子レンズ用永久磁石に用いる導磁性の強磁性
体継鉄又は磁極片を、電気固有抵抗が20マイクロオー
ム・センチメートル以上とした焼結合金を使用する 請求項1記載の電子レンズ用永久磁石。 3、前記溝は前記継鉄を通る磁束に影響しない方向に備
える 請求項1記載の電子レンズ用永久磁石。 4、前記溝は前記継鉄の半径方向に1個設けた請求項1
記載の電子レンズ用永久磁石。[Claims] 1. For an electron lens in which an electron beam passes through the inner holes of at least two ring-shaped permanent magnets that are magnetized in the Z-axis direction, which is the central axis direction of the ring, and connected in the same magnetic pole direction. In the case of permanent magnets, the inner and outer diameters of adjacent ring-shaped permanent magnets are approximately equal to those of the ring-shaped permanent magnets.
A yoke made of a ferromagnetic material with an arbitrary length in the axial direction is sandwiched between the end faces of both ring-shaped permanent magnets and inserted under pressure to increase the half width of the magnetic flux density distribution on the Z axis. A permanent magnet for an electronic lens, characterized in that the yoke and the ring-shaped permanent magnet are made of a sintered alloy having one or more grooves for taking out the lead wires of the coils built into the ring-shaped permanent magnet. 2. The electronic lens according to claim 1, wherein the magnetically conductive ferromagnetic yoke or magnetic pole piece used in the electronic lens permanent magnet is made of a sintered alloy having an electric resistivity of 20 microohm-cm or more. permanent magnet. 3. The permanent magnet for an electronic lens according to claim 1, wherein the groove is provided in a direction that does not affect the magnetic flux passing through the yoke. 4. Claim 1, wherein one groove is provided in the radial direction of the yoke.
Permanent magnet for electronic lenses described.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21035188A JPH0260035A (en) | 1988-08-24 | 1988-08-24 | Permanent magnet for electron lens |
US07/341,947 US4975668A (en) | 1988-04-26 | 1989-04-20 | Electromagnetic focusing |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21035188A JPH0260035A (en) | 1988-08-24 | 1988-08-24 | Permanent magnet for electron lens |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0260035A true JPH0260035A (en) | 1990-02-28 |
Family
ID=16587958
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP21035188A Pending JPH0260035A (en) | 1988-04-26 | 1988-08-24 | Permanent magnet for electron lens |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0260035A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5506482A (en) * | 1993-08-05 | 1996-04-09 | Mitsubishi Denki Kabushiki Kaisha | Magnetic focusing system with improved symmetry and manufacturability |
-
1988
- 1988-08-24 JP JP21035188A patent/JPH0260035A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5506482A (en) * | 1993-08-05 | 1996-04-09 | Mitsubishi Denki Kabushiki Kaisha | Magnetic focusing system with improved symmetry and manufacturability |
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