JPH0139182B2 - - Google Patents
Info
- Publication number
- JPH0139182B2 JPH0139182B2 JP57101550A JP10155082A JPH0139182B2 JP H0139182 B2 JPH0139182 B2 JP H0139182B2 JP 57101550 A JP57101550 A JP 57101550A JP 10155082 A JP10155082 A JP 10155082A JP H0139182 B2 JPH0139182 B2 JP H0139182B2
- Authority
- JP
- Japan
- Prior art keywords
- metal frame
- cathode ray
- ray tube
- panel
- cooling medium
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J29/00—Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
- H01J29/006—Arrangements for eliminating unwanted temperature effects
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J31/00—Cathode ray tubes; Electron beam tubes
- H01J31/08—Cathode ray tubes; Electron beam tubes having a screen on or from which an image or pattern is formed, picked up, converted, or stored
- H01J31/10—Image or pattern display tubes, i.e. having electrical input and optical output; Flying-spot tubes for scanning purposes
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J7/00—Details not provided for in the preceding groups and common to two or more basic types of discharge tubes or lamps
- H01J7/24—Cooling arrangements; Heating arrangements; Means for circulating gas or vapour within the discharge space
Landscapes
- Cathode-Ray Tubes And Fluorescent Screens For Display (AREA)
- Common Detailed Techniques For Electron Tubes Or Discharge Tubes (AREA)
- Electrodes For Cathode-Ray Tubes (AREA)
- Vessels, Lead-In Wires, Accessory Apparatuses For Cathode-Ray Tubes (AREA)
Description
本発明は陰極線管装置、特に例えばカラープロ
ジエクターに用いる高輝度陰極線管に適用して好
適な陰極線管装置に係わる。
高輝度陰極線管は、螢光面に衝撃させる電子ビ
ームのエネルギーを大きくして高い輝度の再生光
学像を得るようにしているが、この場合、螢光面
への電子ビームの衝撃によつて或いはこれに加え
て、例えば螢光面に対向して管体内に、電子ビー
ムの螢光面に対する電子ビームのランデイング位
置を規制するシヤドウマスク、アパーチヤグリル
等の電子ビーム到達位置決定用電極を設ける場合
においてはこの電極に対する電子ビームの衝撃に
よつて発生する熱が電子ビームのエネルギーの増
大化で、より著しくなる。ところが、陰極線管管
体の螢光面が形成された前面パネル、即ちガラス
パネルは、その熱伝導度が低いので、特に連続動
作時において熱の放散がしにくい前面パネル中央
における温度上昇が著しい。そのため螢光体にい
わゆる温度消光が生じる。この温度消光とは温度
の上昇に伴つて螢光体の輝度が低下する現象であ
るが、この温度消光は、各色の螢光面に関してそ
の度合いが異なるのでホワイトバランスに狂いを
生じさせる。
そしてこの中央でのホワイトバランスの狂いは
著しく画質を阻害するので、この中央で連続動作
時ホワイトバランスがとれるように各色の光学像
の輝度を調整することが考えられるが、この場合
は周辺のホワイトバランスが崩れると共に全体の
明るさを高めることができないという欠点が生じ
る。
このことは例えばカラープロジエクターにおい
て各単色の陰極線管より得た各色の画像をスクリ
ーン上に合成投射してカラー画像を得る場合にお
いても、また或いは複数の色の画像によるカラー
画像を同一陰極線管に得て、スクリーン上に投射
するようにしたものの何れにおいても問題となる
ところである。
そこでこの種高輝度陰極線管において、連続動
作によつても、その螢光面に温度消光を生じさせ
るような温度上昇を来すことがないようにするに
はその前面パネルを冷却させる必要がある。この
冷却は冷却フアンによつてなすことが考えられる
が、この場合、管体の前面パネル面に対する送風
と共にパネル面に塵埃を送り込むことになり、こ
の塵埃がパネル面に被着して見掛け上輝度劣化を
来す。またこの場合、冷却フアンの騒音の問題も
生じる。
このような欠点を回避するものとして陰極線管
管体の前面パネルに接して透明液状冷却媒体、特
に対流の生じ易い液体を配してその冷却を行うよ
うにするものが提案された。
このような液冷式陰極線管装置、特に密閉対流
型の陰極線管装置は、例えば第1図にその一部を
断面として示した側面図を示すように、陰極線管
1の前面パネルの前方に例えばガラスより成る光
透過性の透明パネル2を、両パネル1a及び2間
の周辺部にリング状の熱伝導性に優れた金属枠3
を介存させて、この金属枠3によつてパネル1a
及び2間の間隔を設定して対向配置させて成る。
この金属枠3とパネル1aの外面及びパネル2の
内面との間には樹脂接着剤4によつて接着される
と共に液密に封止されてパネル2及び1a間に液
密空間5が形成され、この液密空間5内に透明且
つ対流の生じ易い液状冷媒6が封入充填される。
このような構成による陰極線管管体1は、その
パネル1aがほぼ垂直状態となるようにして動作
される。
この場合、密閉空間5内に充填された冷却媒体
6は、陰極線管管体1の前面パネル1aに熱的に
密に配置される。したがつてこのような構成によ
れば、パネル1aに温度上昇が生じるとこれによ
つて熱せられた冷却媒体6が上方に移行し、これ
が空間5内において対流を生じる。これによつて
パネル1aの例えば中央部の熱といえどもこれが
効果的に周辺部に移行され、この周辺部に配され
た熱伝導性に優れた例えばアルミニウムより成る
金属枠3にその熱が伝達されこの金属枠3中を伝
達して金属枠の外気と接触する外周部から熱の放
散が行われる。
このような構成による陰極線管装置によればパ
ネル1aにおける温度上昇の抑制が比較的効果的
に行われる。
ところが近時、例えばプロジエクタにおいて、
その陰極線管の高輝度、高解像度化が要求され、
高輝度化に伴う高パワー化が要求され、益々効果
的な放熱が要求されるに至つている。更に、この
高パワー化(パワーPは、P=Vp×Ikで与えら
れる。ここにVpは陽極電圧(加速電圧)、Ikはカ
ソード電流である。)に伴つてその加速電圧が高
められると、管体1の前面パネルは、X線透過率
の増加を回避するために、その厚さを大にする必
要が生じる。ところがプロジエクタにおいては、
その光学系において特にプラスチツクレンズを使
用する場合、レンズ設計の上から、螢光面7とレ
ンズとの距離、すなわち前面パネル1aの厚さは
余り大にすることができない。そこで、この場合
は、透明パネル2のガラス素材としてX線の遮蔽
効果を有する例えば鉛の含有量を増加させるとい
う方法が採られることになる。ところがこのよう
に鉛を多量に含むガラスは、その硬度が低下し、
傷つき易くなる性質となる。したがつて、この場
合、前述したような温度上昇が生じて透明パネル
2に熱膨脹によるたわみなどの変形が生じると、
特に破損が生じ易くなる。したがつて、高輝度化
に伴つてより効果的な放熱冷却が要求される。
これがため例えば第1図に示した従来構造のも
のにおいて、例えば放熱フインを設けるなどして
その外気と接触表面積を大にするが、このように
してもその熱放散は差程効果的に行われない。本
発明者等は種々の実験考察を行つた結果、これは
この金属枠3に冷却媒体6の熱が効果的に伝達さ
れていないことによることを究明した。即ち、実
際上金属枠3は、その両パネル2及び1a間に介
存される部分の両外面及び内面が樹脂4によつて
パネル2及び1aと液密に接着されるようになさ
れているために、この金属枠3の冷却媒体6と接
触する面積が小さく、これがため金属枠3に冷却
媒体6の熱が効果的に伝達されていないことを究
明した。
本発明においては、この究明に基づいて冷却媒
体の熱が金属枠に効果的に伝達するように考慮し
たものである。
第2図以下を参照して本発明による陰極線管装
置、即ち密閉対流型の液冷式陰極線管装置の一例
を説明する。
本発明においては第2図に示すように陰極線管
管体1の螢光面7が内面に形成された前面パネル
1aの外面の、有効画面の周囲に金属枠10を配
置し、この金属枠10を介してガラス板等の透明
パネル11を前面パネル1aに所要の間隔を保持
して対向させて、両パネル11及び1a間に液密
空間12を形成するものであるが、特に金属枠1
0を後に詳細に説明する特殊の構成とする。金属
枠10はシリコン樹脂等の接着性樹脂13によつ
て夫々透明パネル11及び前面パネル1aに液密
に密着されると共にパネル1aに金属枠10と透
明パネル11とを機械的に接合する。
透明パネル11と前面パネル1a間の液密空間
12内には液状冷却媒体23、例えばエチレング
リコール水溶液を注入充填する。
金属枠10は、第3図にその正面図を示し第4
図にその側面図を、また第5図に第3図のA−A
線上の断面図を示すように、熱伝導性すぐれた例
えばアルミニウムのダイキヤストよりなり、陰極
線管管体1の前面パネル1aと透明パネル11と
の間の周辺部に介存されて接着性樹脂13との共
働によつてパネル1aとパネル11との間隔を規
制するスペーサとなり陰極線管管体の前面パネル
1aの輪郭形状に対応する輪郭形状を有する枠状
部10aと、これより管体1の前方周面部1a1の
外周に沿つて屈曲するリング状周壁部10bと、
更にその例えば相対向する辺より外側すなわち管
軸とほぼ直交する方向に屈曲し、陰極線管1のキ
ヤビネツト等への取付けに供する取付けねじ孔1
4を有するフランジ部10cと、更にまた、例え
ばこのフランジ部10cを有する部分においてこ
のフランジ部10cと直交する方向に平行植立さ
れた複数の放熱フイン10dとを有して成る。そ
して特に本発明においては、このパネル11と前
面パネル1a間に介存されて両者間の間隔を規制
する枠部10a、即ち接着性樹脂13によつてパ
ネル11及び1aに接着される部分より内側に、
この枠部10aの肉厚より小なる肉厚を有する板
状突出部10eを枠部10aのほぼ全内周に亘つ
て内方向に突出させる。この突出部10eは接着
性樹脂13が接着されることがないようにし更
に、この接着性樹脂13の厚み分の存在によつ
て、或いは及びこの突出部10eが肉薄にされた
ことによつて、そのパネル11と1aと対向する
各面がこれらパネル11及び1aと夫々間隙を保
持して対向するようになされてそのほとんどの部
分が冷却媒体23中に浸漬されて、突出部10e
のほとんどの表面が冷却媒体23と直接的に接触
するようになされる。この突出部10eは枠部1
0aのほぼ全内周に亘つて設けられるが、図示の
例では空間12内に冷却媒体23を注入する注入
孔15が設けられる部分において突出部10eの
欠除部10fが設けられている場合で、突出部1
0eはこの欠除部10fを除いて枠部10aの全
内周に突出して設けられている。
また、この金属枠10は第3図に符号aを付し
て示す有効画面位置より外方にその突出部10e
が存在するようになすが、この場合においても、
螢光面7からの光が金属枠10の例えば突出部1
0eにおいて反射して光学像を乱すことがないよ
うに、少くともその突出部10eの表面を黒化す
る。この黒化処理は、実際上は金属枠10のほと
んど全表面に行つてその熱放射、更に冷却媒体2
3からの吸熱をより効果的に行うようにすること
が望ましい。尚、この黒化処理は、金属枠10が
アルミニウムより成る場合は、アルマイト処理
と、更に必要に応じて染料の使用によつて行い得
る。尚、この場合、黒化処理によつて表面が絶縁
化される場合は、例えば突出部10eの観察、光
学像に影響を与えることのない部分において黒化
処理表面を排除してここにおいて冷却媒体と金属
枠が電気的に連結するようになす。即ち、上述し
たようにグリコール等の透明液状冷却媒体23
は、ある程度の電気伝導性を有するので、この冷
却媒体23と金属枠10とを電気的に連結してお
くことによつてパネル11及び1aを、夫々この
冷却媒体23と金属枠10とを介して例えば接地
することができ、パネル11及び1aの帯電防止
の効果を得ることができる。
また接着性樹脂13は、例えば黒色顔料を含
む、黒色のシリコーン樹脂が用いられる。更に必
要に応じてこのシリコーン樹脂内には、これ自体
がパネル11と前面パネル1a間の間隔を規制す
るスペーサとして金属枠10の枠部10eと共働
してスペーサの効果を得る所要の厚さを確保する
ために、この接着性樹脂13中に既に硬化された
粒状ないしは所要の厚さを有するリング状の弾性
を有する樹脂粒子を混入させておくこともでき
る。
上述の本発明構成によれば、その放熱効果を、
より大とすることができ、これに伴つて陰極線管
のパワーを従来の密閉対流型の液冷式陰極線管装
置におけるそれよりも30%上げて尚現状の信頼性
を維持できることが確められた。即ち、今螢光面
7に印加される陽極電圧Vpを27kVに選定した場
合のカソード電流Ikに対する陰極線管表面におけ
る温度上昇を見ると、本発明においては第6図
中、曲線16に示すようになる。これに比し第1
図で説明した従来構造のものにおいては、即ち、
金属枠に冷却媒体中に浸漬される突出部を設けな
い場合は、曲線17に示すようになり、同じカソ
ード電流において、即ち同パワーとなした場合に
本発明によるそれは従来に比し温度上昇を低く抑
えることができるのでこれに伴つて従来と同様の
温度を許容する状態では、よりパワーの向上が図
られることがわかる。
また、表1に、第1図で説明した従来構造によ
る陰極線管装置の各例(比較例1、2及び3)
と、本発明による陰極線管装置の各例(実施例
1、2、3及び4)の夫々Vp=26kV、Ik=
430μAで連続動作した場合の、その温度が平衡状
態に達した状態での冷却媒体の平均温度の測定結
果を示す。尚、この場合、各例における外気と接
触する放熱面積及び液状冷媒と接触する吸熱面積
は夫々比較例1におけるそれを1として相対的に
示したものであり、実施例1〜4は、夫々金属枠
10の枠部10aの厚さを3.8mmとし、突出部1
0eの厚さを1mmとした場合、実施例1及び2は
突出部10eの突出幅を3mmに、実施例3及び4
のそれは5mmとした場合である。
The present invention relates to a cathode ray tube device, particularly a cathode ray tube device suitable for application to, for example, a high brightness cathode ray tube used in a color projector. In high-brightness cathode ray tubes, the energy of the electron beam that impacts the fluorescent surface is increased to obtain a reproduced optical image with high brightness. In addition to this, for example, when providing an electrode for determining the electron beam arrival position such as a shadow mask or aperture grill for regulating the landing position of the electron beam with respect to the fluorescent surface within the tube facing the fluorescent surface, this is necessary. The heat generated by the impact of the electron beam on the electrode becomes more significant as the energy of the electron beam increases. However, since the front panel of the cathode ray tube body on which the fluorescent surface is formed, ie, the glass panel, has low thermal conductivity, the temperature rises significantly at the center of the front panel, where heat is difficult to dissipate, especially during continuous operation. Therefore, so-called temperature quenching occurs in the phosphor. This temperature quenching is a phenomenon in which the brightness of a phosphor decreases as the temperature rises, and since the degree of temperature quenching differs for each color's phosphor surface, it causes an imbalance in the white balance. Since any deviation in white balance at the center will significantly impede image quality, it may be possible to adjust the brightness of the optical image of each color so that the white balance can be maintained at this center during continuous operation. The disadvantage is that the balance is disrupted and the overall brightness cannot be increased. This applies, for example, when a color image is obtained by combining and projecting each color image obtained from each monochrome cathode ray tube onto a screen in a color projector, or when a color image made up of multiple color images is projected onto the same cathode ray tube. This is a problem in both methods of obtaining images and projecting them onto a screen. Therefore, in this type of high-brightness cathode ray tube, even during continuous operation, it is necessary to cool the front panel in order to prevent the temperature rise that would cause temperature quenching on the fluorescent surface. . This cooling may be done by a cooling fan, but in this case, dust is sent to the front panel surface of the tube along with air, and this dust adheres to the panel surface, causing the apparent brightness to decrease. cause deterioration. In this case, there also arises the problem of noise from the cooling fan. In order to avoid these drawbacks, it has been proposed to cool the cathode ray tube by disposing a transparent liquid cooling medium, especially a liquid that is susceptible to convection, in contact with the front panel of the cathode ray tube. Such a liquid-cooled cathode ray tube device, particularly a closed convection type cathode ray tube device, has, for example, a structure in front of the front panel of the cathode ray tube 1, as shown in a partially sectional side view of FIG. A light-transmissive transparent panel 2 made of glass is surrounded by a ring-shaped metal frame 3 with excellent thermal conductivity around both panels 1a and 2.
With this metal frame 3, the panel 1a is
and are arranged opposite to each other with a set interval between the two.
The metal frame 3 and the outer surface of the panel 1a and the inner surface of the panel 2 are bonded with a resin adhesive 4 and are sealed liquid-tight to form a liquid-tight space 5 between the panels 2 and 1a. The liquid-tight space 5 is filled with a transparent liquid refrigerant 6 that easily causes convection. The cathode ray tube body 1 having such a structure is operated with its panel 1a being in a substantially vertical position. In this case, the cooling medium 6 filled in the closed space 5 is arranged thermally densely on the front panel 1a of the cathode ray tube body 1. Therefore, according to such a configuration, when a temperature rise occurs in the panel 1a, the heated cooling medium 6 moves upward, and this causes convection within the space 5. As a result, even if the heat is in the central part of the panel 1a, it is effectively transferred to the periphery, and the heat is transferred to the metal frame 3 made of aluminum, for example, which has excellent thermal conductivity and is arranged in the periphery. Heat is then transmitted through the metal frame 3 and dissipated from the outer periphery of the metal frame that comes into contact with the outside air. According to the cathode ray tube device having such a configuration, the temperature rise in the panel 1a can be suppressed relatively effectively. However, recently, for example, in projectors,
The cathode ray tube was required to have high brightness and high resolution.
As brightness increases, higher power is required, and more and more effective heat dissipation is required. Furthermore, with this increase in power (power P is given by P = Vp × Ik, where Vp is the anode voltage (acceleration voltage) and Ik is the cathode current), when the acceleration voltage is increased, The thickness of the front panel of the tube body 1 needs to be increased in order to avoid an increase in X-ray transmittance. However, in the projector,
Particularly when a plastic lens is used in the optical system, the distance between the fluorescent surface 7 and the lens, that is, the thickness of the front panel 1a, cannot be made too large due to lens design. Therefore, in this case, a method is adopted in which the content of, for example, lead, which has an X-ray shielding effect, is increased as the glass material of the transparent panel 2. However, the hardness of glass containing a large amount of lead decreases,
It becomes a tendency to be easily hurt. Therefore, in this case, if the temperature rise as described above occurs and the transparent panel 2 undergoes deformation such as deflection due to thermal expansion,
In particular, damage is likely to occur. Therefore, as brightness increases, more effective heat dissipation cooling is required. For this reason, for example, in the conventional structure shown in Fig. 1, the surface area in contact with the outside air is increased by, for example, providing heat dissipation fins, but even with this method, the heat dissipation is not much more effective. do not have. As a result of various experimental studies, the inventors of the present invention have determined that this is because the heat of the cooling medium 6 is not effectively transferred to the metal frame 3. That is, in reality, the metal frame 3 is such that both outer and inner surfaces of the portion interposed between the panels 2 and 1a are liquid-tightly bonded to the panels 2 and 1a by the resin 4. Furthermore, it has been found that the area of the metal frame 3 in contact with the cooling medium 6 is small, and therefore the heat of the cooling medium 6 is not effectively transferred to the metal frame 3. In the present invention, consideration has been given to effectively transmitting the heat of the cooling medium to the metal frame based on this investigation. An example of a cathode ray tube device according to the present invention, that is, a closed convection type liquid-cooled cathode ray tube device, will be described with reference to FIG. 2 and subsequent figures. In the present invention, as shown in FIG. 2, a metal frame 10 is arranged around the effective screen on the outer surface of the front panel 1a on which the fluorescent surface 7 of the cathode ray tube body 1 is formed. A transparent panel 11 such as a glass plate is opposed to the front panel 1a with a required distance therebetween to form a liquid-tight space 12 between the panels 11 and 1a.
0 has a special configuration that will be explained in detail later. The metal frame 10 is liquid-tightly adhered to the transparent panel 11 and the front panel 1a, respectively, by an adhesive resin 13 such as silicone resin, and the metal frame 10 and the transparent panel 11 are mechanically bonded to the panel 1a. A liquid cooling medium 23, such as an ethylene glycol aqueous solution, is injected and filled into the liquid-tight space 12 between the transparent panel 11 and the front panel 1a. The front view of the metal frame 10 is shown in FIG.
The side view is shown in Figure 5, and A-A of Figure 3 is shown in Figure 5.
As shown in the cross-sectional view along the line, the adhesive resin 13 is made of die-cast aluminum having excellent thermal conductivity, and is interposed in the peripheral area between the front panel 1a and the transparent panel 11 of the cathode ray tube body 1. A frame-shaped portion 10a that functions as a spacer to regulate the distance between the panel 1a and the panel 11 and has a contour shape corresponding to the contour shape of the front panel 1a of the cathode ray tube body; a ring-shaped peripheral wall portion 10b bent along the outer periphery of the peripheral surface portion 1a1 ;
Furthermore, there is a mounting screw hole 1 which is bent outward from the opposing sides, that is, in a direction substantially perpendicular to the tube axis, and is used for mounting the cathode ray tube 1 to a cabinet or the like.
4, and a plurality of heat dissipation fins 10d, which are erected in parallel in a direction orthogonal to the flange 10c, for example, in a portion having the flange 10c. In particular, in the present invention, a frame portion 10a that is interposed between the panel 11 and the front panel 1a to regulate the distance between the two, that is, a portion that is bonded to the panels 11 and 1a by the adhesive resin 13 is located on the inner side. To,
A plate-like protruding portion 10e having a wall thickness smaller than that of the frame portion 10a is made to protrude inwardly over substantially the entire inner circumference of the frame portion 10a. This protrusion 10e prevents the adhesive resin 13 from being adhered, and furthermore, by the presence of the thickness of the adhesive resin 13, or by making the protrusion 10e thin, Each surface facing the panels 11 and 1a is made to face the panels 11 and 1a with a gap therebetween, and most of the surfaces are immersed in the cooling medium 23, so that the protrusion 10e
most of the surface is in direct contact with the cooling medium 23. This protruding portion 10e is the frame portion 1
Although it is provided over almost the entire inner circumference of the projection 10a, in the illustrated example, the cutout 10f of the protrusion 10e is provided at a portion where the injection hole 15 for injecting the cooling medium 23 into the space 12 is provided. , protrusion 1
0e is provided so as to protrude from the entire inner periphery of the frame portion 10a except for this cutout portion 10f. Further, this metal frame 10 has a protrusion 10e extending outward from the effective screen position indicated by the symbol a in FIG.
exists, but even in this case,
The light from the fluorescent surface 7 hits the protrusion 1 of the metal frame 10, for example.
At least the surface of the protrusion 10e is blackened so that the light does not disturb the optical image by being reflected at 0e. This blackening treatment is actually performed on almost the entire surface of the metal frame 10, and the heat radiation and the cooling medium 2
It is desirable to absorb heat from 3 more effectively. Incidentally, when the metal frame 10 is made of aluminum, this blackening treatment can be performed by alumite treatment and, if necessary, by using a dye. In this case, if the surface is insulated by the blackening treatment, for example, the blackening treatment surface is removed in a portion that does not affect the observation of the protrusion 10e or the optical image, and the cooling medium is applied here. and the metal frame are electrically connected. That is, as described above, the transparent liquid cooling medium 23 such as glycol
has a certain degree of electrical conductivity, so by electrically connecting the cooling medium 23 and the metal frame 10, the panels 11 and 1a can be connected via the cooling medium 23 and the metal frame 10, respectively. For example, the panels 11 and 1a can be grounded, and the effect of preventing static electricity on the panels 11 and 1a can be obtained. Further, as the adhesive resin 13, for example, a black silicone resin containing a black pigment is used. Furthermore, if necessary, this silicone resin may have a required thickness that functions as a spacer itself to regulate the distance between the panel 11 and the front panel 1a, working together with the frame portion 10e of the metal frame 10 to obtain the spacer effect. In order to ensure this, it is also possible to mix already hardened granular or ring-shaped elastic resin particles with a required thickness into the adhesive resin 13. According to the above-described configuration of the present invention, the heat dissipation effect is
It was confirmed that it was possible to increase the power of the cathode ray tube by 30% over that of conventional closed convection liquid-cooled cathode ray tube devices and still maintain the current reliability. . That is, looking at the temperature rise on the surface of the cathode ray tube with respect to the cathode current Ik when the anode voltage Vp applied to the fluorescent surface 7 is selected to be 27 kV, in the present invention, as shown in curve 16 in FIG. Become. Compared to this, the first
In the conventional structure explained in the figure, namely,
When the metal frame is not provided with a protrusion that is immersed in the cooling medium, it becomes as shown in curve 17. At the same cathode current, that is, at the same power, the temperature rise according to the present invention is lower than that of the conventional method. It can be seen that since the temperature can be kept low, the power can be further improved in a state where the temperature is allowed to be the same as in the conventional case. Table 1 also shows examples of cathode ray tube devices with the conventional structure explained in FIG. 1 (Comparative Examples 1, 2, and 3).
and Vp=26kV, Ik= for each example (Examples 1, 2, 3, and 4) of the cathode ray tube device according to the present invention, respectively.
The results of measuring the average temperature of the cooling medium when operating continuously at 430 μA and when the temperature reaches an equilibrium state are shown. In this case, the heat dissipation area in contact with the outside air and the heat absorption area in contact with the liquid refrigerant in each example are shown relative to that in Comparative Example 1 as 1, and in Examples 1 to 4, metal The thickness of the frame portion 10a of the frame 10 is 3.8 mm, and the protruding portion 1
When the thickness of the protrusion 10e is 1 mm, in Examples 1 and 2, the protrusion width of the protrusion 10e is 3 mm, and in Examples 3 and 4.
This is when the diameter is 5 mm.
【表】【table】
【表】
この表から明らかなように、本発明による場
合、放熱面積を大とするに伴つて放熱効果が上
り、冷却媒体の温度上昇が抑えられる。
上述したように本発明構成によれば、透明パネ
ル11と陰極線管管体1の前面パネル1aとの間
に介存させる金属枠10に液状冷媒と接触する突
出部10eを設け、かつこれを肉薄とし、この肉
薄の突出部10eの全面、すなわち前後両面が冷
却媒体23に浸漬できるようにしたので突出部1
0e、したがつて金属枠10の冷却媒体23との
接触面積の拡大化をはかることができ、これによ
つて格段的に放熱効果を高めることができ、これ
に伴つて陰極線管のパワーを上げることができ、
より高い高輝度陰極線管を得ることができる。特
に前述したようにカラープロジエクターにおいて
は、温度上昇の抑制に伴つて温度消光の発生を回
避でき、ホワイトバランスに狂いのない、即ち色
純度が高く且つ明るいカラー再生画像を得る。ま
た、上述したように、突出部10eを液状冷却媒
体23に浸漬させてその放熱効果を高めるように
したことよつて突出部10eの突出面積の縮小化
をはかることができて、画面の無効部分の縮小
化、ひいて陰極線管装置は全体の小型化をはかる
ことができるという実用上の大きな効果を有す
る。
また金属枠10に黒化処理を施し、特に液状冷
媒内に浸漬する如く突出する突出部の少くとも前
方より観察される側において黒化処理が施こされ
るようにしたので、コントラストの向上更に不要
な光の反射による画質の低下を効果的に回避でき
るものである。[Table] As is clear from this table, in the case of the present invention, the heat radiation effect increases as the heat radiation area increases, and the temperature rise of the cooling medium is suppressed. As described above, according to the configuration of the present invention, the metal frame 10 interposed between the transparent panel 11 and the front panel 1a of the cathode ray tube body 1 is provided with the protrusion 10e that contacts the liquid refrigerant, and this is made thin. Since the entire surface of the thin protrusion 10e, that is, both the front and back surfaces, can be immersed in the cooling medium 23, the protrusion 1
0e, therefore, it is possible to expand the contact area of the metal frame 10 with the cooling medium 23, thereby significantly increasing the heat dissipation effect, and thereby increasing the power of the cathode ray tube. It is possible,
Higher brightness cathode ray tubes can be obtained. In particular, as mentioned above, in a color projector, the occurrence of temperature quenching can be avoided by suppressing the temperature rise, and a reproduced image with bright color and high color purity without any deviation in white balance can be obtained. Furthermore, as described above, by immersing the protrusion 10e in the liquid cooling medium 23 to enhance its heat dissipation effect, the protrusion area of the protrusion 10e can be reduced, and the ineffective area of the screen can be reduced. The cathode ray tube device has the great practical effect of being able to be downsized, and thus the entire cathode ray tube device can be downsized. Further, the metal frame 10 is subjected to a blackening treatment, and in particular, the blackening treatment is applied to at least the side of the protrusion that protrudes as if immersed in the liquid refrigerant and is observed from the front, thereby improving the contrast and This effectively avoids deterioration in image quality due to unnecessary reflection of light.
第1図は従来の密閉対流型の液冷式陰極線管装
置の一部を断面とする側面図、第2図は本発明装
置による陰極線管装置の一例の断面図、第3図は
その金属枠の正面図、第4図はその側面図、第5
図は第3図のA−A線上の断面図、第6図は温度
特性曲線図である。
1は陰極線管管体、1aはその前面パネル、7
は螢光面、11は透明パネル、10は金属枠、1
0eはその突出部、23は液状冷却媒体である。
Fig. 1 is a partially sectional side view of a conventional closed convection type liquid-cooled cathode ray tube device, Fig. 2 is a sectional view of an example of a cathode ray tube device according to the present invention, and Fig. 3 is a metal frame thereof. Figure 4 is its front view, Figure 4 is its side view, and Figure 5 is its side view.
The figure is a sectional view taken along line A--A in FIG. 3, and FIG. 6 is a temperature characteristic curve diagram. 1 is a cathode ray tube body, 1a is its front panel, 7
1 is a fluorescent surface, 11 is a transparent panel, 10 is a metal frame, 1
0e is its protrusion, and 23 is a liquid cooling medium.
Claims (1)
の周囲に金属枠が配され、該金属枠を介して透明
パネルが、上記前面パネルに対して上記金属枠に
よつて規定される間隔をもつて対向されて上記前
面パネルと上記透明パネルとの間に液密空間が形
成され、該液密空間内に透明液状冷却媒体が封入
され、上記透明パネルと上記前面パネルとの上記
液密空間に臨む上記金属枠の内周端部に、上記液
状冷却媒体内に浸漬され該液状冷却媒体と全面に
亘つて接触する上記金属枠の肉厚より薄い肉厚を
有する突出部が上記金属体枠と一体に設けられて
成る陰極線管装置。1. A metal frame is arranged around the effective screen on the outer surface of the front panel of the cathode ray tube body, and a transparent panel is inserted through the metal frame at a distance defined by the metal frame with respect to the front panel. A liquid-tight space is formed between the front panel and the transparent panel facing each other, a transparent liquid cooling medium is sealed in the liquid-tight space, and a liquid-tight space between the transparent panel and the front panel is sealed. A protruding portion having a wall thickness thinner than a wall thickness of the metal frame that is immersed in the liquid cooling medium and comes into contact with the liquid cooling medium over the entire surface is provided on the inner circumferential end of the metal frame facing the metal body frame. A cathode ray tube device that is integrated.
Priority Applications (8)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57101550A JPS58218734A (en) | 1982-06-14 | 1982-06-14 | Cathode-ray tube device |
| CA000429864A CA1205509A (en) | 1982-06-14 | 1983-06-07 | Cathode ray tube apparatus |
| AU15617/83A AU564241B2 (en) | 1982-06-14 | 1983-06-08 | Cathode ray tube cooling apparatus |
| KR1019830002572A KR900003216B1 (en) | 1982-06-14 | 1983-06-09 | Cathode-ray tube |
| GB08315993A GB2124425B (en) | 1982-06-14 | 1983-06-10 | Liquid cooled cathode ray tubes |
| DE3321489A DE3321489A1 (en) | 1982-06-14 | 1983-06-14 | LIQUID-COOLED IMAGE DISPLAY DEVICE |
| FR8309833A FR2528624B1 (en) | 1982-06-14 | 1983-06-14 | CATHODE RAY TUBE IN PARTICULAR FOR A CATHODE RAY |
| NL8302119A NL8302119A (en) | 1982-06-14 | 1983-06-14 | LIQUID COOLED CATHODE JET TUBE. |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57101550A JPS58218734A (en) | 1982-06-14 | 1982-06-14 | Cathode-ray tube device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58218734A JPS58218734A (en) | 1983-12-20 |
| JPH0139182B2 true JPH0139182B2 (en) | 1989-08-18 |
Family
ID=14303532
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57101550A Granted JPS58218734A (en) | 1982-06-14 | 1982-06-14 | Cathode-ray tube device |
Country Status (8)
| Country | Link |
|---|---|
| JP (1) | JPS58218734A (en) |
| KR (1) | KR900003216B1 (en) |
| AU (1) | AU564241B2 (en) |
| CA (1) | CA1205509A (en) |
| DE (1) | DE3321489A1 (en) |
| FR (1) | FR2528624B1 (en) |
| GB (1) | GB2124425B (en) |
| NL (1) | NL8302119A (en) |
Families Citing this family (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58154146A (en) * | 1982-03-10 | 1983-09-13 | Sony Corp | Liquid cooling type cathode-ray tube |
| JPS59157938A (en) * | 1983-02-24 | 1984-09-07 | Sony Corp | Cathode ray tube device |
| JPS603548U (en) * | 1983-06-20 | 1985-01-11 | ソニー株式会社 | cathode ray tube device |
| EP0162972B1 (en) * | 1984-06-01 | 1988-10-05 | Philips Patentverwaltung GmbH | Projection cathode ray tube |
| JPS62169448U (en) * | 1986-04-17 | 1987-10-27 | ||
| JPH0658474B2 (en) * | 1989-09-04 | 1994-08-03 | カシオ計算機株式会社 | Liquid crystal display |
Family Cites Families (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US2241974A (en) * | 1938-04-05 | 1941-05-13 | Gen Electric | High power cathode ray device |
| JPS597731Y2 (en) * | 1979-06-07 | 1984-03-09 | ソニー株式会社 | cathode ray tube equipment |
| JPS57180957U (en) * | 1981-05-12 | 1982-11-16 | ||
| JPS58154145A (en) * | 1982-03-09 | 1983-09-13 | Sony Corp | Cathode-ray tube |
| JPS58154146A (en) * | 1982-03-10 | 1983-09-13 | Sony Corp | Liquid cooling type cathode-ray tube |
| JPS58182250U (en) * | 1982-05-28 | 1983-12-05 | 日本電気ホームエレクトロニクス株式会社 | projection cathode ray tube |
-
1982
- 1982-06-14 JP JP57101550A patent/JPS58218734A/en active Granted
-
1983
- 1983-06-07 CA CA000429864A patent/CA1205509A/en not_active Expired
- 1983-06-08 AU AU15617/83A patent/AU564241B2/en not_active Expired
- 1983-06-09 KR KR1019830002572A patent/KR900003216B1/en not_active Expired
- 1983-06-10 GB GB08315993A patent/GB2124425B/en not_active Expired
- 1983-06-14 FR FR8309833A patent/FR2528624B1/en not_active Expired
- 1983-06-14 NL NL8302119A patent/NL8302119A/en active Search and Examination
- 1983-06-14 DE DE3321489A patent/DE3321489A1/en not_active Ceased
Also Published As
| Publication number | Publication date |
|---|---|
| FR2528624B1 (en) | 1986-10-10 |
| AU564241B2 (en) | 1987-08-06 |
| GB2124425B (en) | 1986-03-26 |
| FR2528624A1 (en) | 1983-12-16 |
| DE3321489A1 (en) | 1983-12-15 |
| CA1205509A (en) | 1986-06-03 |
| GB8315993D0 (en) | 1983-07-13 |
| NL8302119A (en) | 1984-01-02 |
| KR900003216B1 (en) | 1990-05-10 |
| GB2124425A (en) | 1984-02-15 |
| JPS58218734A (en) | 1983-12-20 |
| AU1561783A (en) | 1983-12-22 |
| KR840005275A (en) | 1984-11-05 |
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