WO2003019607A1 - Funnel glass for cathode ray tube - Google Patents
Funnel glass for cathode ray tube Download PDFInfo
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- WO2003019607A1 WO2003019607A1 PCT/JP2002/008467 JP0208467W WO03019607A1 WO 2003019607 A1 WO2003019607 A1 WO 2003019607A1 JP 0208467 W JP0208467 W JP 0208467W WO 03019607 A1 WO03019607 A1 WO 03019607A1
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- Prior art keywords
- glass
- ray tube
- cathode ray
- funnel glass
- funnel
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- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03C—CHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
- C03C3/00—Glass compositions
- C03C3/04—Glass compositions containing silica
- C03C3/076—Glass compositions containing silica with 40% to 90% silica, by weight
- C03C3/102—Glass compositions containing silica with 40% to 90% silica, by weight containing lead
- C03C3/105—Glass compositions containing silica with 40% to 90% silica, by weight containing lead containing aluminium
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- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03C—CHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
- C03C4/00—Compositions for glass with special properties
- C03C4/08—Compositions for glass with special properties for glass selectively absorbing radiation of specified wave lengths
- C03C4/087—Compositions for glass with special properties for glass selectively absorbing radiation of specified wave lengths for X-rays absorbing glass
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- 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
- H01J29/86—Vessels; Containers; Vacuum locks
- H01J29/863—Vessels or containers characterised by the material thereof
Definitions
- the present invention relates to a funnel glass for a cathode ray tube.
- the cathode ray tube envelope includes a panel glass on which an image is projected, a tubular neck glass on which an electron gun is mounted, and a funnel-shaped funnel glass connecting the panel glass and the neck glass.
- Phosphor is coated on the inner surface of the panel glass to display images.
- the inner and outer surfaces of each of the neck glass and the funnel glass are coated with a carbon conductive film (carbon doug) in order to equalize the potential inside the cathode ray tube bulb when generating an electron beam from the electron gun.
- a cathode ray tube In a cathode ray tube, when an applied voltage is applied to the anode, an electron beam is emitted from the electron gun, which is a cathode, and the phosphor attached to the inner surface of the panel glass emits light to display an image on the panel glass. At this time, braking X-rays are generated in the cathode ray tube. Damping X-rays leaking out of the tube through the envelope can have an adverse effect on the human body. For this reason, this type of envelope is required to have high X-ray absorption capacity.
- the light emitted from the phosphor mainly passes through the panel glass to display an image, but part of the light goes to the funnel side and enters the funnel glass.
- the amount of light generated from the phosphor is particularly large, and therefore, the amount of light entering the funnel glass is also large.
- the glass used as the conventional funnel glass is almost colorless and transparent, and the light transmittance at a wavelength of 450-650 nm is about 85% with a glass thickness of 10 mm. Therefore, light that has entered the funnel glass may repeatedly diffuse and reflect on the inner and outer surfaces of the glass and reach the panel glass.
- the panel glass and the funnel glass are welded to the direct without any frit, so that light is easily guided from the funnel glass to the panel glass.
- the light guided to the panel glass mixes with the image light, causing a problem of reducing the contrast of the image.
- an object of the present invention is to provide a funnel glass for a cathode ray tube, which can prevent a decrease in the contrast of the cathode ray tube. Disclosure of the invention
- the present inventor has found that by reducing the light transmittance in the visible region of the funnel glass for a cathode ray tube, the absorption of light penetrating the glass is increased, and the decrease in the contrast of the cathode ray tube is suppressed. I found that I could do it.
- the light transmittance in a wavelength range of 450 to 65 nm is 80% or less at a glass thickness of 10 mm, and at a wavelength of 0.06 nm.
- X-ray absorption coefficient of 40 cm- 1 or more is obtained.
- the light transmittance in the wavelength range of 450 to 65 nm is set to 80% or less with a glass thickness of 10 mm.
- the X-ray absorption coefficient at a wavelength of 0.06 nm is set to 40 cm- 1 or more.
- this funnel glass Since this funnel glass has a light transmittance of 80% or less, it has an excellent light absorbing effect. For this reason, of the light emitted from the phosphor attached to the inner surface of the panel glass, the light that has entered the funnel glass is gradually absorbed into the glass while being repeatedly reflected on the inner and outer surfaces of the funnel glass. Therefore, it is necessary to reduce light that is guided from the panel glass to the panel glass and mixed into the image light. And a decrease in contrast can be prevented.
- the transmittance of the glass is more than 80%, the effect of absorbing light is reduced, so that light mixed into the panel glass cannot be reduced, and the contrast is undesirably reduced.
- the preferred light transmittance is 60% or less, more preferably 50% or less.
- At least one colorant selected from the group consisting of CuO and MnO may be contained in a total amount of 10 to 50,000 ppm. If the total amount of the coloring agent is less than 10 ppm, the effect of lowering the transmittance of the glass is reduced. If the total amount is more than 50,000 ppm, the meltability of the glass is deteriorated.
- the preferred range of the total amount of the colorant is 20 to 30,000 ppm.
- the funnel glass for a cathode ray tube has a high X-ray absorption coefficient at 0.6 A of 40 cm- 1 or more, so that X-rays do not leak outside the tube.
- compositions usable in this funnel glass in percent by mass, S I_ ⁇ 2 48 ⁇ 58%, A 1 2 0 3 0. 5 ⁇ 6%, PbO 10 ⁇ 30%, MgO 0 ⁇ 5%, CaO Less than six%, S R_ ⁇ 0 to 9%, B A_ ⁇ 0 to 9%, Na 2 ⁇ 3 ⁇ 9%, K 2 0 4 ⁇ ll %, Sb 2 0 3 0 ⁇ 1%, colorant 10 It is in the range of 50000 ppm, and it may be selected so as to satisfy the above conditions within this range.
- the reasons for limiting the glass composition as described above are as follows.
- S i ⁇ 2 is a component that becomes a glass network former.
- the content of Si ⁇ 2 is 48 to 58% by mass, the molding of the funnel glass becomes easy, and the consistency with the thermal expansion coefficient of the neck glass is improved.
- the preferred range of the funnel glass is 50-57% by mass.
- a 1 2 ⁇ 3 is also a component that becomes the network former of glass. If the amount of A 1 2 0 3 is 0.5 to 6% by weight, molding of the funnel glass is facilitated, the tooth may, better consistency between the thermal expansion coefficient of the neck glass.
- the preferred range of A 1 2 0 3 is from 1 to 5 mass%.
- PbO is a component that increases the X-ray absorption coefficient of glass. When the content of PbO is 10 to 30% by mass, a sufficient X-ray absorption capacity can be obtained, and the viscosity can be adjusted to a value suitable for molding funnel glass.
- the preferred range of Pb ⁇ is 15 to 27% by mass.
- Mg ⁇ is a component that adjusts the coefficient of thermal expansion and viscosity while making glass easier to melt.
- MgO is 5% by mass or less, the glass is not easily devitrified, and the liquidus temperature is lowered, so that funnel glass is easily molded.
- Mg 0 is preferably at most 4% by mass.
- Ca ⁇ is also a component that adjusts the coefficient of thermal expansion and the viscosity while making glass easier to melt, like MgO.
- the content of Ca ⁇ is 6% by mass or less, the glass is hardly devitrified and the liquidus temperature is lowered, so that funnel glass is easily molded.
- the preferred range of C a0 is 1 to 5% by mass.
- each of SrO and BaO is 9 When the content is less than 10% by mass, the glass is less likely to be devitrified, and the liquidus temperature is lowered, so that funnel glass can be easily formed.
- Each of 1 " ⁇ and 8 & ⁇ is preferably 7% by mass, respectively. It is as follows.
- Na 2 ⁇ is a component that adjusts the coefficient of thermal expansion and viscosity.
- the content of Na 2 3 is 3 to 9% by mass, the consistency with the thermal expansion coefficient of the neck glass is improved, and the viscosity can be adjusted to be suitable for molding the funnel glass.
- a preferred range of N a 2 0 is 4-8 wt%.
- K 2 ⁇ also a component that adjusts the thermal expansion coefficient and viscosity as well as the N a 2 0.
- the content of K 20 is 4 to 11% by mass, the consistency with the thermal expansion coefficient of the neck glass is improved, and the viscosity can be adjusted to be suitable for molding the funnel glass.
- the preferred range of ⁇ 2 ⁇ is 5 to 10% by mass.
- Sb 2 ⁇ 3 is a component which acts as a fining agent.
- Sb 2 ⁇ 3 is preferably 0.05 to 0.8 wt%.
- the cathode-ray tube funnel glass in addition to the above components, as impurities resulting from the raw materials used, ZnO, that each of Z r0 2, T I_ ⁇ 2, F e 2 0 3 including multi Kutomo 2% it can.
- the light transmittance is defined based on a glass thickness of 1 Omm, but it goes without saying that the present invention can be applied to any funnel glass having various thicknesses.
- Table 1 shows examples of the present invention (sample Nos. 1 to 4) and comparative examples (sample No. 5).
- Each sample in the table was prepared as follows First, glass raw materials were prepared so as to have the composition shown in the table, and were melted at 1500 ° C. for 4 hours using a platinum pot. In order to obtain a homogeneous glass, degassing was performed by stirring for 3 minutes on the way. Thereafter, the molten glass was poured into a mold, formed into a predetermined shape, and gradually cooled.
- the X-ray absorption coefficient was obtained by calculating the absorption coefficient for a wavelength of 0.06 nm based on the glass composition and density.
- the transmittance As for the transmittance, after optical polishing was performed so that the glass thickness became 10 mm, the light transmittance at a wavelength of 450 to 650 nm was measured with a spectrophotometer, and the maximum transmittance was shown in the table.
- the average coefficient of thermal expansion at 30 to 380 ° C was measured with a dilatometer.
- the temperature was measured at which the viscosity of the glass corresponds to 10 4 dP a ⁇ s by platinum ball pulling method.
- This molding temperature is a guide when molding the molten glass into a predetermined shape, and the lower the temperature, the better the moldability.
- each sample was first ground and mixed to a size of 300 to 500 m, mixed, placed in a platinum port, transferred to a temperature gradient furnace at 800 to 1200 ° C, and held for 48 hours. Then, a port made of platinum was taken out of the temperature gradient furnace. Then, the glass was taken out of the platinum port. The sample thus obtained was observed with a polarizing microscope, and the crystal precipitation point was measured.
- each of the samples No. 1 to No. 4 has a high X-ray absorption coefficient of 66 cm- 1 or more, so that X-rays generated inside the cathode ray tube can be shielded.
- the maximum transmittance of glass with a wavelength of 450 to 650 nm was as low as 55% or less.
- the thermal expansion coefficient of 101 X 10- 7 Z ° C the panel can be well matched with glass Ya net Kugarasu, molding temperature 966 ° C below the liquidus temperature is lower than 890 ° C, glass Was also excellent in moldability.
- the sample of sample No. 5 has the highest wavelength of 450-650 nm glass.
- the large transmittance was as high as 84%.
- the funnel glass prepared from each of Sample Nos.! To No. 4 is superior to the funnel glass prepared from Sample No. 5 in the effect of absorbing light. It can be assumed that it is possible to reduce the light mixed into the panel glass and prevent the contrast from decreasing. Industrial applicability
- the funnel glass for a cathode ray tube of the present invention is suitable as a glass used for manufacturing a funnel for a cathode ray tube.
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- Chemical & Material Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Engineering & Computer Science (AREA)
- Chemical Kinetics & Catalysis (AREA)
- General Chemical & Material Sciences (AREA)
- Geochemistry & Mineralogy (AREA)
- Materials Engineering (AREA)
- Organic Chemistry (AREA)
- Glass Compositions (AREA)
- Vessels, Lead-In Wires, Accessory Apparatuses For Cathode-Ray Tubes (AREA)
Abstract
Description
明 細 書 陰極線管用ファンネルガラス 技術分野 Description Funnel glass for cathode ray tube Technical field
本発明は、 陰極線管用ファンネルガラスに関するものである。 背景技術 The present invention relates to a funnel glass for a cathode ray tube. Background art
陰極線管の外囲器は、 映像が映し出されるパネルガラスと、 電子銃が装着さ れる管状のネックガラスと、 パネルガラスとネックガラスを接続する漏斗状の ファンネルガラスとを含んでいる。 パネルガラスの内面には、 映像を映し出す ために蛍光体が塗布されている。 ネックガラス及びファンネルガラスの各々の 内外表面には、 電子銃から電子線を発生させる際に陰極線管バルブ内の電位を 同じにするために、 カーボンの導電膜 (カーボンダグ) が塗布されている。 陰極線管は、 陽極に印加電圧をかけると、 陰極である電子銃から電子線が出 てパネルガラスの内面に付けた蛍光体を発光させてパネルガラスに映像を映し 出す。 この時に制動 X線が陰極線管内に発生する。 制動 X線は外囲器を通して 管外に漏れると人体に悪影響を及ぼす。 このため、 この種の外囲器には高い X 線吸収能を有することが要求されている。 The cathode ray tube envelope includes a panel glass on which an image is projected, a tubular neck glass on which an electron gun is mounted, and a funnel-shaped funnel glass connecting the panel glass and the neck glass. Phosphor is coated on the inner surface of the panel glass to display images. The inner and outer surfaces of each of the neck glass and the funnel glass are coated with a carbon conductive film (carbon doug) in order to equalize the potential inside the cathode ray tube bulb when generating an electron beam from the electron gun. In a cathode ray tube, when an applied voltage is applied to the anode, an electron beam is emitted from the electron gun, which is a cathode, and the phosphor attached to the inner surface of the panel glass emits light to display an image on the panel glass. At this time, braking X-rays are generated in the cathode ray tube. Damping X-rays leaking out of the tube through the envelope can have an adverse effect on the human body. For this reason, this type of envelope is required to have high X-ray absorption capacity.
ところで、 蛍光体から発する光は、 主にパネルガラスを通過し映像を映し出 すが、 一部はファンネル側に向かい、 ファンネルガラス内に侵入する。 例えば 投射型陰極線管の場合には、 陽極に高い電圧及び電流が印加されるため、 蛍光 体から発生する光の量が特に多くなり、 したがってファンネルガラス内に侵入 する光の量も多くなる。 By the way, the light emitted from the phosphor mainly passes through the panel glass to display an image, but part of the light goes to the funnel side and enters the funnel glass. For example, in the case of a projection type cathode ray tube, since a high voltage and current are applied to the anode, the amount of light generated from the phosphor is particularly large, and therefore, the amount of light entering the funnel glass is also large.
従来のファンネルガラスとして用いられているガラスは、 殆ど無色透明であ り、 波長 4 5 0〜6 5 0 n mにおける光透過率は、 ガラス肉厚 1 0 mmで、 お よそ 8 5 %である。 そのため、 ファンネルガラス内に侵入した光は、 ガラスの 内外表面で拡散、 反射を繰り返してパネルガラスに達することがある。 特に投 射型陰極線管の場合、 パネルガラスとファンネルガラスとは、 フリットを介在 させることなく、 ダイレク卜に熔着されるため、 ファンネルガラスからパネル ガラスに光が導かれやすい。 パネルガラスに導かれた光は、 映像光に混ざり、 映像のコントラストを低下させるという問題を引き起こす。 The glass used as the conventional funnel glass is almost colorless and transparent, and the light transmittance at a wavelength of 450-650 nm is about 85% with a glass thickness of 10 mm. Therefore, light that has entered the funnel glass may repeatedly diffuse and reflect on the inner and outer surfaces of the glass and reach the panel glass. Especially In the case of a projection cathode ray tube, the panel glass and the funnel glass are welded to the direct without any frit, so that light is easily guided from the funnel glass to the panel glass. The light guided to the panel glass mixes with the image light, causing a problem of reducing the contrast of the image.
それ故に本発明の目的は、 陰極線管のコントラスト低下を防止することが可 能な陰極線管用ファンネルガラスを提供することである。 発明の開示 Therefore, an object of the present invention is to provide a funnel glass for a cathode ray tube, which can prevent a decrease in the contrast of the cathode ray tube. Disclosure of the invention
本発明者は、 種々の実験を繰り返した結果、 陰極線管用ファンネルガラスの 可視域における光透過率を低下させることによって、 ガラスに侵入した光の吸 収性を高め、 陰極線管のコントラスト低下を抑えることができることを見いだ した。 As a result of repeating various experiments, the present inventor has found that by reducing the light transmittance in the visible region of the funnel glass for a cathode ray tube, the absorption of light penetrating the glass is increased, and the decrease in the contrast of the cathode ray tube is suppressed. I found that I could do it.
本発明の一態様によれば、 波長 4 5 0〜6 5 0 n mの範囲における光透過率 が、 ガラス肉厚 1 0 mmで、 8 0 %以下であり、 且つ、 波長 0 . 0 6 n mおけ る X線吸収係数が 4 0 c m—1以上であることを特徴とする陰極線管用フアンネ ルガラスが得られる。 発明を実施するための最良の形態 According to one embodiment of the present invention, the light transmittance in a wavelength range of 450 to 65 nm is 80% or less at a glass thickness of 10 mm, and at a wavelength of 0.06 nm. X-ray absorption coefficient of 40 cm- 1 or more is obtained. BEST MODE FOR CARRYING OUT THE INVENTION
以下、 本発明の実施例に係る陰極線管用ファンネルガラスについて説明する。 ここで説明する陰極線管用ファンネルガラスは、 波長 4 5 0〜6 5 0 n mの 範囲における光透過率が、 ガラス肉厚 1 0 mmで、 8 0 %以下に設定されてい る。 しかも、 波長 0 . 0 6 n mおける X線吸収係数は 4 0 c m— 1以上に設定さ れている。 Hereinafter, a funnel glass for a cathode ray tube according to an embodiment of the present invention will be described. In the funnel glass for a cathode ray tube described here, the light transmittance in the wavelength range of 450 to 65 nm is set to 80% or less with a glass thickness of 10 mm. Moreover, the X-ray absorption coefficient at a wavelength of 0.06 nm is set to 40 cm- 1 or more.
このファンネルガラスは、 光透過率が 8 0 %以下であるため、 光を吸収する 作用に優れている。 このため、 パネルガラスの内面に付けた蛍光体から発する 光のうち、 ファンネルガラス内へ侵入した光は、 ファンネルガラスの内外表面 で反射を繰り返す間に、 徐々にガラス中に吸収される。 したがって、 フアンネ ルガラスからパネルガラスに導かれて、 映像光に混入する光を減少させること ができ、 コントラストの低下を防止することができる。 Since this funnel glass has a light transmittance of 80% or less, it has an excellent light absorbing effect. For this reason, of the light emitted from the phosphor attached to the inner surface of the panel glass, the light that has entered the funnel glass is gradually absorbed into the glass while being repeatedly reflected on the inner and outer surfaces of the funnel glass. Therefore, it is necessary to reduce light that is guided from the panel glass to the panel glass and mixed into the image light. And a decrease in contrast can be prevented.
ガラスの透過率が 80 %より大きいと、 光を吸収する作用が小さくなり、 パ ネルガラスに混入する光を減少させることができず、 コン卜ラス卜が低下する ため好ましくない。 好ましい光透過率は 60%以下であり、 より好ましくは 5 0 %以下である。 If the transmittance of the glass is more than 80%, the effect of absorbing light is reduced, so that light mixed into the panel glass cannot be reduced, and the contrast is undesirably reduced. The preferred light transmittance is 60% or less, more preferably 50% or less.
ファンネルガラスの波長 450〜650 nmの光透過率を 80 %以下にする には、 例えば、 ガラス中に Co 304、 N i〇、 C r 203、 V2〇5、 S e02、 CuO、 及び MnOの群から選択された少なくとも一種の着色剤を合量で、 1 0〜50000 p pm含有させればよい。 着色剤の合量が 10 p pmより少な いと、 ガラスの透過率を低下させる効果が小さくなり、 50000 ppmより 多いと、 ガラスの熔融性が悪化する。 着色剤の合量の好ましい範囲は 20〜3 0000 p pmである。 The light transmittance at a wavelength of 450 to 650 nm of the funnel glass to below 80%, for example, Co 3 0 4 in the glass, N I_〇, C r 2 0 3, V 2 〇 5, S e0 2, At least one colorant selected from the group consisting of CuO and MnO may be contained in a total amount of 10 to 50,000 ppm. If the total amount of the coloring agent is less than 10 ppm, the effect of lowering the transmittance of the glass is reduced. If the total amount is more than 50,000 ppm, the meltability of the glass is deteriorated. The preferred range of the total amount of the colorant is 20 to 30,000 ppm.
また、 この陰極線管用ファンネルガラスは、 0. 6Aにおける X線吸収係数 が 40 cm—1以上と高いため、 X線が管外に漏れることがない。 The funnel glass for a cathode ray tube has a high X-ray absorption coefficient at 0.6 A of 40 cm- 1 or more, so that X-rays do not leak outside the tube.
このファンネルガラスに使用可能な具体的組成は、 質量百分率で、 S i〇2 48〜58%、 A 1203 0. 5〜6%、 PbO 10〜30%、 MgO 0 〜5%、 CaO 0〜6%、 S r〇 0〜9 %、 B a〇 0〜9 %、 Na2〇 3 〜9%、 K20 4〜l l%、 Sb 203 0〜1%、 着色剤 10〜50000 p pmの範囲であり、 この範囲内で上記条件を満たすように選択すればよい。 ガラスの組成を上記のように限定した理由は、 次のとおりである。 Specific compositions usable in this funnel glass, in percent by mass, S I_〇 2 48~58%, A 1 2 0 3 0. 5~6%, PbO 10~30%, MgO 0 ~5%, CaO Less than six%, S R_〇 0 to 9%, B A_〇 0 to 9%, Na 2 〇 3 ~9%, K 2 0 4~ll %, Sb 2 0 3 0~1%, colorant 10 It is in the range of 50000 ppm, and it may be selected so as to satisfy the above conditions within this range. The reasons for limiting the glass composition as described above are as follows.
S i〇 2は、 ガラスのネットワークフォーマーとなる成分である。 S i〇2の 含有量が 48〜58質量%のとき、 ファンネルガラスの成型が容易になり、 し かも、 ネックガラスの熱膨張係数との整合性が良くなる。 ファンネルガラスの 好ましい範囲は 50〜57質量%である。 S i〇 2 is a component that becomes a glass network former. When the content of Si 含有2 is 48 to 58% by mass, the molding of the funnel glass becomes easy, and the consistency with the thermal expansion coefficient of the neck glass is improved. The preferred range of the funnel glass is 50-57% by mass.
A 12〇3もガラスのネットワークフォーマ一となる成分である。 A 1203の 含有量が 0. 5〜6質量%のとき、 ファンネルガラスの成型が容易になり、 し かも、 ネックガラスの熱膨張係数との整合性が良くなる。 A 1203の好ましい 範囲は 1〜 5質量%である。 PbOは、 ガラスの X線吸収係数を高める成分である。 PbOの含有量が 1 0〜30質量%のとき、 十分な X線吸収能力を得ることができ、 しかも、 ファ ンネルガラスの成型に適した粘度にすることができる。 P b〇の好ましい範囲 は 15〜27質量%である。 A 1 2 〇 3 is also a component that becomes the network former of glass. If the amount of A 1 2 0 3 is 0.5 to 6% by weight, molding of the funnel glass is facilitated, the tooth may, better consistency between the thermal expansion coefficient of the neck glass. The preferred range of A 1 2 0 3 is from 1 to 5 mass%. PbO is a component that increases the X-ray absorption coefficient of glass. When the content of PbO is 10 to 30% by mass, a sufficient X-ray absorption capacity can be obtained, and the viscosity can be adjusted to a value suitable for molding funnel glass. The preferred range of Pb〇 is 15 to 27% by mass.
Mg〇は、 ガラスを熔融しやすくすると共に、 熱膨張係数と粘度を調整する 成分である。 MgOの含有量が5質量%以下のとき、 ガラスが失透しにくく、 液相温度が低くなるためファンネルガラスの成型が容易となる。 M g 0は好ま しくは 4質量%以下である。 Mg〇 is a component that adjusts the coefficient of thermal expansion and viscosity while making glass easier to melt. When the content of MgO is 5% by mass or less, the glass is not easily devitrified, and the liquidus temperature is lowered, so that funnel glass is easily molded. Mg 0 is preferably at most 4% by mass.
Ca〇も MgOと同様にガラスを熔融しやすくすると共に、 熱膨張係数と粘 度を調整する成分である。 C a〇の含有量が 6質量%以下のとき、 ガラスが失 透しにくく、 液相温度が低くなるためファンネルガラスの成型が容易となる。 C a 0の好ましい範囲は 1〜 5質量%である。 Ca〇 is also a component that adjusts the coefficient of thermal expansion and the viscosity while making glass easier to melt, like MgO. When the content of Ca〇 is 6% by mass or less, the glass is hardly devitrified and the liquidus temperature is lowered, so that funnel glass is easily molded. The preferred range of C a0 is 1 to 5% by mass.
31"〇と8 &0は、 ガラスを熔融しやすくすると共に、 熱膨張係数と粘度を 調整し、 さらに X線吸収能を高める成分である。 S r Oと B aOの各々の含有 量がそれぞれ 9質量%以下のとき、 ガラスが失透しにくく、 液相温度が低くな るためファンネルガラスの成型が容易となる。 3 1"〇と8 &〇の各々は、 好ま しくは、 それぞれ 7質量%以下である。 31 ”〇 and 8 & 0 are components that facilitate melting of glass, adjust the coefficient of thermal expansion and viscosity, and further enhance X-ray absorption. The content of each of SrO and BaO is 9 When the content is less than 10% by mass, the glass is less likely to be devitrified, and the liquidus temperature is lowered, so that funnel glass can be easily formed. 3 Each of 1 "〇 and 8 & 〇 is preferably 7% by mass, respectively. It is as follows.
Na2〇は、 熱膨張係数と粘度を調整する成分である。 Na2〇の含有量が 3 〜9質量%のとき、ネックガラスの熱膨張係数との整合性が良くなり、 しかも、 ファンネルガラスの成型に適した粘度にすることができる。 N a 20の好ましい 範囲は 4〜8質量%である。 Na 2 〇 is a component that adjusts the coefficient of thermal expansion and viscosity. When the content of Na 2 3 is 3 to 9% by mass, the consistency with the thermal expansion coefficient of the neck glass is improved, and the viscosity can be adjusted to be suitable for molding the funnel glass. A preferred range of N a 2 0 is 4-8 wt%.
K2〇も N a 20と同様に熱膨張係数と粘度を調整する成分である。 K20の含 有量が 4〜11質量%のとき、 ネックガラスの熱膨張係数との整合性も良くな り、 しかも、 ファンネルガラスの成型に適した粘度にすることができる。 Κ2〇 の好ましい範囲は 5〜10質量%である。 K 2 〇 also a component that adjusts the thermal expansion coefficient and viscosity as well as the N a 2 0. When the content of K 20 is 4 to 11% by mass, the consistency with the thermal expansion coefficient of the neck glass is improved, and the viscosity can be adjusted to be suitable for molding the funnel glass. The preferred range of { 2 } is 5 to 10% by mass.
Sb2〇3は、 清澄剤として働く成分である。 S b203が多くなると、 ガラス が失透しやすくなるが、 1質量%までの添加であれば問題はない。 Sb2〇3は、 好ましくは、 0. 05〜0. 8質量%である。 さらに、 この陰極線管用ファンネルガラスは、 上記成分以外にも、 用いる原 料から生じる不純物として、 ZnO、 Z r02、 T i〇2、 F e 203の各々を多 くとも 2%含むことができる。 Sb 2 〇 3 is a component which acts as a fining agent. When the S b 2 0 3 increases, but the glass tends to be devitrified, no problem as long as the addition of up to 1% by weight. Sb 2 〇 3 is preferably 0.05 to 0.8 wt%. Furthermore, the cathode-ray tube funnel glass, in addition to the above components, as impurities resulting from the raw materials used, ZnO, that each of Z r0 2, T I_〇 2, F e 2 0 3 including multi Kutomo 2% it can.
尚、 上述ではガラス肉厚 1 Ommを基準にして光透過率を規定しているが、 本発明は様々な肉厚をもつファンネルガラスにいずれも適用され得ることは言 うまでもない。 In the above description, the light transmittance is defined based on a glass thickness of 1 Omm, but it goes without saying that the present invention can be applied to any funnel glass having various thicknesses.
表 1は本発明の実施例 (試料 No. 1〜4) と比較例 (試料 No. 5) を示 すものである。 Table 1 shows examples of the present invention (sample Nos. 1 to 4) and comparative examples (sample No. 5).
表中の各試料は、 次のようにして作製した まず、 表の組成となるようにガラス原料を調合し、 白金ポットを用いて 15 00°Cで 4時間溶融した。 尚、 均質なガラスを得るため、 途中で 3分間攪拌し て脱泡を行った。 その後、 溶融ガラスを金型に流し出して所定形状に成形し、 徐冷した。 Each sample in the table was prepared as follows First, glass raw materials were prepared so as to have the composition shown in the table, and were melted at 1500 ° C. for 4 hours using a platinum pot. In order to obtain a homogeneous glass, degassing was performed by stirring for 3 minutes on the way. Thereafter, the molten glass was poured into a mold, formed into a predetermined shape, and gradually cooled.
このようにして得られた各試料について、 X線吸収係数、 透過率、 熱膨張係 数、 成型温度及び液相温度を測定し、 表に示した。 The X-ray absorption coefficient, transmittance, thermal expansion coefficient, molding temperature and liquidus temperature of each sample thus obtained were measured and are shown in the table.
尚、 X線吸収係数は、 ガラス組成と密度に基づいて、 0. 06 nmの波長に 対する吸収係数を計算して求めたものである。 The X-ray absorption coefficient was obtained by calculating the absorption coefficient for a wavelength of 0.06 nm based on the glass composition and density.
透過率は、 ガラスの肉厚が 10mmとなるように光学研磨を行った後、 分光 光度計によって、 波長 450〜 650 nmの光透過率を測定し、 最大透過率を 表に示した。 As for the transmittance, after optical polishing was performed so that the glass thickness became 10 mm, the light transmittance at a wavelength of 450 to 650 nm was measured with a spectrophotometer, and the maximum transmittance was shown in the table.
熱膨張係数については、 ディラトメーターで 30〜380°Cにおける平均熱 膨張係数を測定した。 Regarding the coefficient of thermal expansion, the average coefficient of thermal expansion at 30 to 380 ° C was measured with a dilatometer.
成形温度については、 ガラスの粘度が 104dP a · sに相当する温度を白金 球引き上げ法により測定した。 この成形温度が熔融ガラスを所定形状に成形す る際の目安となり、 この温度が低い方が成形性は良い。 For molding temperature, the temperature was measured at which the viscosity of the glass corresponds to 10 4 dP a · s by platinum ball pulling method. This molding temperature is a guide when molding the molten glass into a predetermined shape, and the lower the temperature, the better the moldability.
液相温度については、 まず、 各試料をそれぞれ 300〜500 mの大きさ に粉碎、 混合し、 これを白金製のポートに入れて 800〜1200°Cの温度勾 配炉に移して 48時間保持し、 温度勾配炉より白金製のポートを取り出した。 その後、 白金製のポートからガラスを取り出した。 このようにして得られたサ ンプルを偏光顕微鏡で観察し、 結晶の析出点を測定した。 Regarding the liquidus temperature, each sample was first ground and mixed to a size of 300 to 500 m, mixed, placed in a platinum port, transferred to a temperature gradient furnace at 800 to 1200 ° C, and held for 48 hours. Then, a port made of platinum was taken out of the temperature gradient furnace. Then, the glass was taken out of the platinum port. The sample thus obtained was observed with a polarizing microscope, and the crystal precipitation point was measured.
表から明らかなように、 試料 No. l〜No. 4の各試料は、 X線吸収係数 が 66 cm—1以上と高いため、 陰極線管内部で発生する X線を遮蔽することが できる。 また、 波長 450〜650 nmのガラスの最大透過率は 55 %以下と 低かった。 更に熱膨張係数も 101 X 10— 7Z°Cであり、 パネルガラスゃネッ クガラスと良好に整合することができ、 成型温度は 966°C以下、 液相温度は 890°C以下と低く、 ガラスの成形性にも優れていた。 As is clear from the table, each of the samples No. 1 to No. 4 has a high X-ray absorption coefficient of 66 cm- 1 or more, so that X-rays generated inside the cathode ray tube can be shielded. The maximum transmittance of glass with a wavelength of 450 to 650 nm was as low as 55% or less. Furthermore the thermal expansion coefficient of 101 X 10- 7 Z ° C, the panel can be well matched with glass Ya net Kugarasu, molding temperature 966 ° C below the liquidus temperature is lower than 890 ° C, glass Was also excellent in moldability.
これに対し、 試料 No. 5の試料は、 波長 450〜650 nmのガラスの最 大透過率が 84 %と高かった。 On the other hand, the sample of sample No. 5 has the highest wavelength of 450-650 nm glass. The large transmittance was as high as 84%.
上記の結果から、 試料 No. ;!〜 No. 4の各試料から作製したファンネル ガラスは、 試料 No. 5の試料から作製したファンネルガラスに比べて、 光を 吸収する作用に優れているため、 パネルガラスに混入する光を減少させ、 コン トラストの低下を防止することが可能であると推測できる。 産業上の利用可能性 From the above results, the funnel glass prepared from each of Sample Nos.! To No. 4 is superior to the funnel glass prepared from Sample No. 5 in the effect of absorbing light. It can be assumed that it is possible to reduce the light mixed into the panel glass and prevent the contrast from decreasing. Industrial applicability
本発明の陰極線管用ファンネルガラスは、 陰極線管用ファンネルの製造に使 用するガラスとして好適である。 The funnel glass for a cathode ray tube of the present invention is suitable as a glass used for manufacturing a funnel for a cathode ray tube.
Claims
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2001-253282 | 2001-08-23 | ||
| JP2001253282A JP2003068233A (en) | 2001-08-23 | 2001-08-23 | Funnel glass for cathode-ray tube |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| WO2003019607A1 true WO2003019607A1 (en) | 2003-03-06 |
Family
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| PCT/JP2002/008467 Ceased WO2003019607A1 (en) | 2001-08-23 | 2002-08-22 | Funnel glass for cathode ray tube |
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| Country | Link |
|---|---|
| JP (1) | JP2003068233A (en) |
| CN (1) | CN1255848C (en) |
| WO (1) | WO2003019607A1 (en) |
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| CN107814483A (en) * | 2017-12-04 | 2018-03-20 | 滕州市耀海玻雕有限公司 | One kind energy-conservation fire resistance hollow glass and its manufacture method |
| CN120004504B (en) * | 2025-02-18 | 2025-11-18 | 成都光明光电股份有限公司 | Optical glass and glass element |
Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5844656A (en) * | 1981-09-09 | 1983-03-15 | Hitachi Ltd | projection type cathode ray tube |
| JPH07206469A (en) * | 1993-12-08 | 1995-08-08 | Philips Electron Nv | Glass used in display tube cone, display tube envelope having cone of said glass and method of producing cone from said glass |
| JP2000086279A (en) * | 1998-07-10 | 2000-03-28 | Asahi Glass Co Ltd | Glass for cathode ray tube funnel |
| JP2000323071A (en) * | 1999-05-13 | 2000-11-24 | Nippon Electric Glass Co Ltd | Funnel glass for cathode-ray tube |
| JP2001052632A (en) * | 1999-08-13 | 2001-02-23 | Nippon Electric Glass Co Ltd | Neck glass for cathode-ray tube |
| JP2001148225A (en) * | 1999-09-07 | 2001-05-29 | Nippon Electric Glass Co Ltd | Cathode ray tube and method of manufacturing cathode ray tube |
-
2001
- 2001-08-23 JP JP2001253282A patent/JP2003068233A/en active Pending
-
2002
- 2002-08-22 WO PCT/JP2002/008467 patent/WO2003019607A1/en not_active Ceased
- 2002-08-22 CN CN 02816445 patent/CN1255848C/en not_active Expired - Fee Related
Patent Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5844656A (en) * | 1981-09-09 | 1983-03-15 | Hitachi Ltd | projection type cathode ray tube |
| JPH07206469A (en) * | 1993-12-08 | 1995-08-08 | Philips Electron Nv | Glass used in display tube cone, display tube envelope having cone of said glass and method of producing cone from said glass |
| JP2000086279A (en) * | 1998-07-10 | 2000-03-28 | Asahi Glass Co Ltd | Glass for cathode ray tube funnel |
| JP2000323071A (en) * | 1999-05-13 | 2000-11-24 | Nippon Electric Glass Co Ltd | Funnel glass for cathode-ray tube |
| JP2001052632A (en) * | 1999-08-13 | 2001-02-23 | Nippon Electric Glass Co Ltd | Neck glass for cathode-ray tube |
| JP2001148225A (en) * | 1999-09-07 | 2001-05-29 | Nippon Electric Glass Co Ltd | Cathode ray tube and method of manufacturing cathode ray tube |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2003068233A (en) | 2003-03-07 |
| CN1545719A (en) | 2004-11-10 |
| CN1255848C (en) | 2006-05-10 |
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