JPH01144547A - Focus magnet - Google Patents
Focus magnetInfo
- Publication number
- JPH01144547A JPH01144547A JP30212887A JP30212887A JPH01144547A JP H01144547 A JPH01144547 A JP H01144547A JP 30212887 A JP30212887 A JP 30212887A JP 30212887 A JP30212887 A JP 30212887A JP H01144547 A JPH01144547 A JP H01144547A
- Authority
- JP
- Japan
- Prior art keywords
- magnet
- flux density
- magnetic flux
- permanent magnets
- focus
- 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.)
- Granted
Links
- 230000005291 magnetic effect Effects 0.000 claims abstract description 38
- 230000004907 flux Effects 0.000 claims abstract description 19
- 229910000859 α-Fe Inorganic materials 0.000 claims description 3
- 230000005415 magnetization Effects 0.000 abstract 1
- 238000010894 electron beam technology Methods 0.000 description 9
- 230000010287 polarization Effects 0.000 description 8
- 230000000694 effects Effects 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- 230000004075 alteration Effects 0.000 description 2
- 229910000828 alnico Inorganic materials 0.000 description 1
- 239000000571 coke Substances 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 239000003302 ferromagnetic material Substances 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 150000002739 metals Chemical class 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2例えばビデオプロジェクタ−1投射型高品位
テレビ等に使用する投射型ブラウン管用のフォーカスマ
グネットに関するものであり、特に高精細プロジェクタ
−用のフォーカスマグネットの改良に関するものである
。[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a focus magnet for a projection type cathode ray tube used in, for example, a video projector-1 projection type high-definition television, etc., and particularly relates to a focus magnet for a high-definition projector. The present invention relates to an improvement of the focus magnet.
従来電子銃から発射された電子ビームを螢光面上に収束
する装置としては、静電方式のものが使用されており、
X線管、マグネトロン、進行波管等の特殊管用には、磁
界方式が使用されていた。Conventionally, an electrostatic type device has been used to focus the electron beam emitted from an electron gun onto a fluorescent surface.
Magnetic field methods were used for special tubes such as X-ray tubes, magnetrons, and traveling wave tubes.
しかし最近では高品位テレビ等解像度の高いものが要求
される結果、磁界方式に移行しつつある。However, as a result of the recent demand for high-resolution devices such as high-definition televisions, there is a shift toward magnetic field methods.
而して磁界方式の1つである電磁石方式のものでは、大
形であると共に電源を必要とする欠点があるため、永久
磁石によるものが中心となっている。The electromagnet type, which is one type of magnetic field type, has the drawbacks of being large and requiring a power source, and therefore permanent magnets are mainly used.
第2図はその一例を示すもので、軸方向に着磁して端面
にN、S磁極を設け、中空円筒形に形成した永久磁石1
の両端面に2強磁性材料からなり。Figure 2 shows an example of this. A permanent magnet 1 is magnetized in the axial direction and has N and S magnetic poles on the end face, and is formed into a hollow cylindrical shape.
Consists of two ferromagnetic materials on both end faces.
かつ中空に形成したコーク2を固着して磁気回路を形成
すると共に、永久磁石1の内周にボビン4を介してコイ
ル3を介装させたものである。上記のように形成して、
リード線(図示せず)を介してコイル3に通電すれば、
永久磁石1による中心磁界を調整することができ、中心
軸上の電子ビームを収束する作用が期待できるのである
。A magnetic circuit is formed by fixing a hollow coke 2, and a coil 3 is interposed on the inner circumference of the permanent magnet 1 via a bobbin 4. Form as above,
If the coil 3 is energized via a lead wire (not shown),
The central magnetic field of the permanent magnet 1 can be adjusted, and the effect of converging the electron beam on the central axis can be expected.
上記従来のフォーカスマグネットによる中心軸上の電子
ビームを収束したスポット径は0.3〜0.350であ
るが、最近の高精細プロジェクタ−用としては、上記ス
ポット径は0.25〜0.28mが要求されている。し
かし従来のフォーカスマグネットにおいて電子ビームの
スポット径を絞ろうとしても1球面収差が大きく、ハレ
ーションが現れるという欠点がある。この欠点を解消す
るために、少なくとも2個のリング状永久磁石を同一磁
極方向に連結し、これらの永久磁石のZ軸上の磁束密度
分布の半値幅を永久磁石の内径の80%〜200%とす
る内容の提案がされている(特開昭61−211940
号公報参照)。この提案は、リング状に形成した永久磁
石のZ軸上の磁束分布の半値幅Bwと永久磁石の内径り
との比、すなわちH= B w / Lの値をパラメー
タとし、Hを大幅に増大させるためには別個に着磁され
、同一磁極方向に少なくとも2個のリング状永久磁石を
連結した構成とすることが有効であること、および球面
収差を改善するためには上記Hを0.8以上にすれば好
ましいことを内容とするものである。The spot diameter of the converged electron beam on the central axis by the conventional focus magnet is 0.3 to 0.350 m, but for recent high-definition projectors, the spot diameter is 0.25 to 0.28 m. is required. However, in conventional focusing magnets, even if an attempt is made to narrow down the spot diameter of the electron beam, one spherical aberration is large and halation occurs. In order to eliminate this drawback, at least two ring-shaped permanent magnets are connected in the same magnetic pole direction, and the half-value width of the magnetic flux density distribution on the Z axis of these permanent magnets is set to 80% to 200% of the inner diameter of the permanent magnet. It has been proposed that the content of
(see publication). This proposal uses the ratio of the half width Bw of the magnetic flux distribution on the Z axis of a ring-shaped permanent magnet to the inner diameter of the permanent magnet, that is, the value of H = B w / L, as a parameter, and significantly increases H. In order to achieve this, it is effective to have a configuration in which at least two ring-shaped permanent magnets are magnetized separately and connected in the same magnetic pole direction, and in order to improve spherical aberration, the above H should be set to 0.8. The content above is what is preferable.
前記の高精細プロジェクタ−用のフォーカスマグネット
に要求される性能としては、Z軸上の磁束密度、磁束密
度の半値幅、軸ずれ、楕円率、偏磁率等において極めて
高度のものが要求されている。ここにおいて偏磁率とは
1例えばフォーカスマグネットを保持するホルダー内径
の中心から径方向に10m離れた仮想円筒面(直径20
m)上における軸方向磁束密度の最大点および最小点で
の磁束密度のバラツキであり、3%以下と規定される場
合がある。このような性能を要求されるフォーカスマグ
ネットにおいて、前記のようにHの値を大きく設定する
と、偏磁率が大きくなり、電子ビームの良好な集束がで
きなくなるという問題点がある。The performance required of the focus magnet for the above-mentioned high-definition projector is extremely high in terms of magnetic flux density on the Z-axis, half-width of magnetic flux density, axis misalignment, ellipticity, polarization, etc. . Here, the magnetic polarization is 1. For example, a virtual cylindrical surface (diameter 20
m) is the variation in the magnetic flux density at the maximum and minimum points of the axial magnetic flux density on the axial direction, and may be specified as 3% or less. In a focus magnet that is required to have such performance, if the value of H is set to a large value as described above, there is a problem in that the magnetic polarization increases, making it impossible to focus the electron beam well.
本発明は、上記従来技術の問題点を解決し、Z軸上の磁
束密度、半値幅を確保しつつ、偏磁率が小さく電子ビー
ムの集束性能の高いフォーカスマグネットを提供するこ
とを目的とする。SUMMARY OF THE INVENTION An object of the present invention is to solve the above-mentioned problems of the prior art, and to provide a focus magnet that has a small polarization and high electron beam focusing performance while ensuring the magnetic flux density and half-width on the Z-axis.
上記従来技術の問題点を解決するために9本発明におい
ては、軸方向に着磁して両端面に磁極を設け、この磁極
面に中空円板状のヨークを固着してなる少なくとも2個
の中空円筒形の永久磁石を。In order to solve the above-mentioned problems of the prior art, the present invention provides at least two magnetic poles, which are magnetized in the axial direction and provided with magnetic poles on both end faces, and a hollow disk-shaped yoke is fixed to the magnetic pole faces. A hollow cylindrical permanent magnet.
異極を対向させて同軸上に連結してなるフォーカスマグ
ネットにおいて、永久磁石の2軸上の磁束密度分布の半
値幅を、永久磁石の内径の40〜80%とする。という
技術的手段を採用したのである。In a focus magnet formed by coaxially connecting different poles facing each other, the half width of the magnetic flux density distribution on two axes of the permanent magnet is set to 40 to 80% of the inner diameter of the permanent magnet. This technical method was adopted.
第1図は本発明の実施例を示す要部断面図であり、同一
部分は前記第2図と同一の参照符号で示す、同図におい
て2個の永久磁石1,1は各々異極を対向させ、かつヨ
ーク2を介して同軸上に結合固着させる。なお永久磁石
1.1の内周にはボビン4を介してコイル3を介装させ
る。次に永久磁石1をフェライト磁石(日立金属製YB
M−2B)により形成し、磁束密度の半値幅Bwおよび
内径りを種々変化させて、Z軸上の磁束密度Bzおよび
偏磁率δを測定した結果を表に示す。FIG. 1 is a cross-sectional view of essential parts showing an embodiment of the present invention, and the same parts are designated by the same reference numerals as in FIG. and are coaxially coupled and fixed via the yoke 2. Note that a coil 3 is interposed on the inner circumference of the permanent magnet 1.1 via a bobbin 4. Next, permanent magnet 1 is a ferrite magnet (YB manufactured by Hitachi Metals)
The table shows the results of measuring the magnetic flux density Bz on the Z axis and the magnetic polarization δ by changing the half width Bw of the magnetic flux density and the inner diameter variously.
表から明らかなように隘1においては、Z軸上の磁束密
度Bzが不足し、フォーカスマグネットとして要求され
る電子ビームの収束機能を満足できない、一方磁7にお
いては、上記磁束密度BzO値は充分であるが、偏磁率
δの値が大きすぎ。As is clear from the table, in No. 1, the magnetic flux density Bz on the Z axis is insufficient and cannot satisfy the electron beam focusing function required for a focus magnet, while in No. 7, the above magnetic flux density BzO value is sufficient. However, the value of magnetic polarization δ is too large.
高精細プロジェクタ−用のフォーカスマグネットに要求
される3%以下という性能を満足していない。これに対
して漱2〜6においては、Z軸上の磁束密度Bzの値も
充分大であり、満足すべき電子ビーム収束機能を保有す
ると共に、偏磁率δの値も小さいため、前記要求機能を
満足していることが認められる。It does not satisfy the performance of 3% or less required for focus magnets for high-definition projectors. On the other hand, in Sō 2 to 6, the value of the magnetic flux density Bz on the Z axis is sufficiently large, and the value of the magnetic polarization δ is small, as well as having a satisfactory electron beam focusing function, so that the above-mentioned required function is achieved. It is recognized that the following are satisfied.
本実施例においては、永久磁石としてフェライト磁石を
・使用した例について記述したが、アルニコ磁石等の鋳
造磁石を使用してもよい。また永久磁石の端面に固着す
べきヨークの構成材料としては、鉄板その他の磁性材料
を適宜選定して使用す、 る。In this embodiment, an example is described in which a ferrite magnet is used as a permanent magnet, but a cast magnet such as an alnico magnet may also be used. Further, as the constituent material of the yoke to be fixed to the end face of the permanent magnet, an iron plate or other magnetic material is appropriately selected and used.
本発明は2以上記述のような構成および作用であるから
、電子ビームの集束性能に寄与するZ軸上の磁束密度お
よび半値幅を充分に大きくし得ると共に、高精細プロジ
ェクタ−用として要求される偏磁率を大幅に低減させる
ことができ、フォーカスマグネットの性能を大幅に向上
し得るという効果がある。Since the present invention has the configuration and operation as described above, it is possible to sufficiently increase the magnetic flux density and half-width on the Z-axis, which contribute to the focusing performance of the electron beam, and also to sufficiently increase the magnetic flux density and half-width, which are required for high-definition projectors. This has the effect that the magnetic polarization can be significantly reduced, and the performance of the focus magnet can be greatly improved.
第1図は本発明の実施例を示す要部断面図、第2図は従
来のフォーカスマグネットの例を示す要部断面図である
。
l:永久磁石、2:ヨーク。FIG. 1 is a sectional view of a main part showing an embodiment of the present invention, and FIG. 2 is a sectional view of a main part showing an example of a conventional focus magnet. l: permanent magnet, 2: yoke.
Claims (2)
面に中空円板状のヨークを固着してなる少なくとも2個
の中空円筒形の永久磁石を、異極を対向させて同軸上に
連結してなるフォーカスマグネットにおいて、永久磁石
のZ軸上の磁束密度分布の半値幅を、永久磁石の内径の
40〜80%としたことを特徴とするフォーカスマグネ
ット。(1) At least two hollow cylindrical permanent magnets are magnetized in the axial direction and have magnetic poles on both end faces, and a hollow disc-shaped yoke is fixed to the magnetic pole faces, with different poles facing each other. A focus magnet connected coaxially, characterized in that the half width of the magnetic flux density distribution on the Z axis of the permanent magnet is 40 to 80% of the inner diameter of the permanent magnet.
第1項記載のフォーカスマグネット。(2) The focus magnet according to claim 1, wherein the permanent magnet is a ferrite magnet.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62302128A JPH07118281B2 (en) | 1987-11-30 | 1987-11-30 | Focus magnet |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62302128A JPH07118281B2 (en) | 1987-11-30 | 1987-11-30 | Focus magnet |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH01144547A true JPH01144547A (en) | 1989-06-06 |
JPH07118281B2 JPH07118281B2 (en) | 1995-12-18 |
Family
ID=17905257
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP62302128A Expired - Lifetime JPH07118281B2 (en) | 1987-11-30 | 1987-11-30 | Focus magnet |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH07118281B2 (en) |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61211940A (en) * | 1985-03-15 | 1986-09-20 | Sony Corp | Permanent magnet for electron lens |
-
1987
- 1987-11-30 JP JP62302128A patent/JPH07118281B2/en not_active Expired - Lifetime
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61211940A (en) * | 1985-03-15 | 1986-09-20 | Sony Corp | Permanent magnet for electron lens |
Also Published As
Publication number | Publication date |
---|---|
JPH07118281B2 (en) | 1995-12-18 |
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