Patent Grant
7075222
This Non-provisional application claims priority under 35 U.S.C. § 119(a) on Patent Application No(s). 10-2003-0041730 filed in Korea on Jun. 25, 2003, the entire contents of which are hereby incorporated by reference.
1. Field of the Invention
The present invention relates to a color cathode ray tube, and more particularly, to a color cathode ray tube capable of obtaining a structural intensity of a mask corresponding to a panel, decreasing a partial doming, and increasing a drop characteristic by setting a curvature of the panel to be greater from a center portion of the panel towards a peripheral portion thereof.
2. Description of the Related Art
Generally, a color cathode ray tube is for implementing images, and is divided into a curved type cathode ray tube and a flat type cathode ray tube according to an appearance of a panel.
The curved type cathode ray tube has several problems such as an image distortion, eyes fatigue due to light reflection, and etc. thus to have decreasing demands, whereas the flat type cathode ray tube has advantages in that images are not distorted, reflection for external light is minimized, and maximization of a visual region can be implemented thus to have increasing demands.
As shown, the conventional color cathode ray tube comprises a panel 1 having a fluorescent surface 1a, a mask 2 for selecting colors of electron beams incident from an inner side of the panel 1, a funnel 3 coupled to a rear surface of the panel 1 for maintaining inside of the cathode ray tube as a vacuum state, an electron gun 5 mounted in a neck portion 4 of the funnel 3 for emitting electron beams, and a deflection yoke 6 for surrounding outside of the funnel 3 and deflecting electron beams.
In the conventional color cathode ray tube, when image signals are inputted to the electron gun 5, the electron gun 5 emits electron beams and the emitted electron beams are accelerated and focused towards the panel 1 according to voltages applied from each electrode of the electron gun 5.
At this time, the electron beams are deflected by the deflection yoke 6 thus to pass slots formed at the mask 2, and thereby colors of the electron beams are selected. Then, the electron beams collide with the fluorescent surface 1a inside the panel 1 thus to make each fluorescent surface 1a emit light, thereby reproducing images.
In the conventional color cathode ray tube, a method for reducing a center thickness of a panel or a method for flattening an inner surface of a panel were used in order to make the cathode ray tube light and to reduce a cost.
However, in the method for reducing a center thickness of a panel, when the center thickness of a panel becomes thinner than a current standard of 10.5 mm, x-ray emission amount is increased thus to have a limitation.
Also, in the method for flattening an inner surface of a panel, the inner surface of a panel becomes gradually flat and thereby a curvature of a mask becomes gradually flat, thereby decreasing a structural intensity of a mask and thus deteriorating a drop quality (a drop characteristic). Also, when the panel mask becomes flat, electron beams which have passed through mask holes do not correctly hit red, green, and blue phosphors of a screen by a thermal expansion of the mask, thereby generating a partial doming that a color purity of a screen is deteriorated.
To prevent said partial doming, in the conventional art, invar steel, a low thermal expansion material instead of AK, a high thermal expansion material was used to fabricate a mask, which was disclosed in Japanese patent 1984-15861.
In case of using a mask of said invar steel material (hereinafter, invar mask), a thermal expansion of a mask can be decreased. However, in this case, the cost is high, a mechanical workability is very poor thus to have an annealing process temperature more than 900° C., and a metallic pattern has to be heated at the time of forming the mask.
Also, the invar mask has a low structural intensity compared to a mask of AK material (AK mask) and causes a drop characteristic deterioration, so that a wedge ratio of a panel (a ratio of a corner thickness of a panel for a center thickness) was set to be 220% or more than and a mask curvature was set to be similar to a spherical type, that is, to be similar to a single curvature radius R in the conventional art. According to this, an optimum curvature of a panel which is light, reduces a fabrication cost, and increases a structural intensity could not be implemented.
Therefore, an object of the present invention is to provide a color cathode ray tube capable of obtaining a structural intensity of a mask corresponding to a panel, decreasing a partial doming, and increasing a drop characteristic by setting a curvature of the panel to be greater from a center portion of the panel towards a peripheral portion thereof.
To achieve these and other advantages and in accordance with the purpose of the present invention, as embodied and broadly described herein, there is provided a color cathode ray tube comprising: a panel of which an outer surface is substantially plane and an inner surface has a predetermined curvature; and a mask for selecting colors of electron beams incident from inside of the panel, in which a formula, 0.3≦(Rxe/Rxc)≦0.75 is satisfied.
The foregoing and other objects, features, aspects and advantages of the present invention will become more apparent from the following detailed description of the present invention when taken in conjunction with the accompanying drawings.
The accompanying drawings, which are included to provide a further understanding of the invention and are incorporated in and constitute a part of this specification, illustrate embodiments of the invention and together with the description serve to explain the principles of the invention.
In the drawings:
Reference will now be made in detail to the preferred embodiments of the present invention, examples of which are illustrated in the accompanying drawings.
Hereinafter, a color cathode ray tube according to the present invention will be explained in more detail.
As shown in
In case of increasing the inner curvature of the panel from the center portion of the panel 10 towards the peripheral portion of the effective surface (hereinafter, a super arc), a structural intensity of a mask corresponding to the inner curvature of the panel can be obtained, thereby effectively solving problems such as a partial doming generated at the time of using an AK mask or a tint panel.
Especially, in the present invention, the partial doming can be more effectively reduced by forming an inner curvature of the panel to be relatively greater than a curvature of the center portion at a ⅔ region from the effective surface center portion towards the peripheral portion of the panel, the weakest region for the partial doming of the cathode ray tube.
Hereinafter, a long axis is defined as a line in the center of the panel parallel to a longer side of the panel, a short axis is defined as a line in the center of the panel parallel to a shorter side of the panel, a Rxe is defined as an inner curvature radius at an edge of a long axis of the panel,
a Rye is defined as an inner curvature radius at edge of a short axis of the panel, a Ryc is defined as an inner curvature radius at a center of a short axis of the panel, a Rxc is defined as an inner curvature radius at a center of a long axis of the panel, a Rdc is defined as an inner curvature radius at a center of a diagonal axis of the panel, a Rde is defined as an inner curvature radius at a edge of a diagonal axis of the panel, and a USD is defined as an effective surface diagonal distance of the panel.
The color cathode ray tube according to the present invention comprises a panel 10 of which an outer surface is substantially plane and an inner surface has a predetermined curvature, a mask 20 for selecting colors of electron beams, a funnel 30 coupled to a rear surface of the panel 10 for maintaining inside of the cathode ray tube as a vacuum state, an electron gun 50 for emitting electron beams, and a deflection yoke 60 for deflecting electron beams. At the time of forming the inner curvature of the panel 10, the panel curvature is increased towards the peripheral portion of the effective surface from the center portion of the panel 10, and a formula, 0.3≦(Rxe/Rxc)≦0.75 is satisfied.
Also, formulas, 4.5≦Rxc/USD≦8.5, 0.3≦Rye/Ryc≦1.0, and Rxe≦Rde≦Rye are satisfied, and the USD is 500 mm or less than.
In the color cathode ray tube of the present invention, a mask of AK material or a mask of invar material can be used. In case of using a mask of AK material, formulas, 0.3≦(Rxe/Rxc)≦0.5, 4.5≦(Rxc/USD)≦8.5, 0.3≦(Rye/Ryc)≦1.0, and Rxe≦Rde≦Rye are preferably satisfied, and the USD is 500 mm or less than. Also, a transmission ratio of the center portion of the panel 10 is 45%˜75%, and the wedge ratio is 180%˜220%.
In case of using a mask of Fe—Ni based alloy invar or a Fe—Ni—Co based alloy ultra invar, formulas, 0.5≦(Rxe/Rxc)≦0.75, 4.5≦(Rxc/USD)≦6.5, 0.3≦(Rye/Ryc)≦1.0, and Rxe≦Rde≦Rye are satisfied, the USD is 500 mm or less than, and the wedge ratio is 200% or more than.
Hereinafter, the super arc ratio of the color cathode ray tube according to the present invention will be explained.
In the conventional color cathode ray tube, the inner curvature radius of the panel is formed as a single R, so that the inner curvature radius from the center portion of the panel to the edge of the effective surface is equal. However, in the color cathode ray tube of the present invention, the inner curvature radius of the panel is formed as a super arc and a mask curvature corresponding to the inner curvature of the panel is designed as a super arc without an infection point, thereby obtaining a structural intensity of the mask, increasing a drop characteristic, and thus reducing a partial doming.
Also, in the color cathode ray tube of the present invention, the curvature value(Z) is drastically increased from the center portion of the panel towards the peripheral portion, which shows that a curvature is drastically increased from the center portion of the panel towards the peripheral portion.
Hereinafter, the AK mask and the invar mask will be explained with comparison each other.
As shown, a thermal expansion of the AK mask is approximately 5 times greater than that of the invar mask, so that a partial doming that a color purity of a screen is deteriorated has to be solved at the time of using the AK mask.
That is, in case of using the invar mask, the partial doming is 20 μm or less than thus not to generate a phenomenon that the color purity of the screen is deteriorated. However, in case of using the AK mask, the partial doming is 70 μm or more than, which corresponds to approximately 3 times of the invar mask in the same curvature mask and causes the color purity of the screen to be deteriorated.
The mask curvature is varied according to the inner curvature of the panel even in case of a mask having the same wedge ratio, so that the inner curvature of the panel has to be designed as a form to reduce the partial doming.
In case of a cathode ray tube using the AK material mask, a drop characteristic and B/U according to the wedge ratio of the panel are shown in a following table 1 and
As shown in the table 1 and
Accordingly, in order to use the AK mask and the tint panel, the wedge ratio of the panel has to be 180%˜220% and the B/U has to be 70˜78 thus to satisfy a required drop characteristic of the CDT.
As shown, in case of a cathode ray tube using an invar mask, the drop characteristic and B/U according to the wedge ratio of the panel are shown in a following table 2 and
As shown in the table 2 and
A following table 3 shows a reducing ratio of the partial doming according to a variance of the curvature radius.
As shown in the table 3, as a measurement result of the partial doming with an invar mask having a thickness of 0.12 mm, when the curvature radius of the panel is varied from 1500 mm to 1100 mm (when a curvature is increased), the partial doming is varied from 21 μm to 14 μm, which means the partial doming is varied nearly similarly to the variation ratio of the curvature radius of the panel. That is, the table 3 shows that the partial doing is decreased accordingly as the inner curvature of the panel is increased.
As can be seen from said result, in order to use the AK mask and the tint panel, the wedge ratio of the panel has to be 180%˜220% thus to satisfy required drop characteristic of the CDT. Also, in case of using the invar mask, the wedge ratio has to be 220% or more than in order to satisfy the drop characteristic.
As shown, the super arc ratio of the inner curvature of the panel along a long axis has to exceed 20% in order to satisfy 30 G(Gravity), the drop characteristic of the cathode ray tube in a wedge ratio of 220% or less than even if a structural intensity of the mask is increased by using the AK material.
In order to decrease the partial doming with 30% or more than, the super arc ratio has to be increased. In this case, a ratio of the inner curvature radius of the effective surface edge for the inner curvature radius of the center portion of the panel along the long axis satisfies a following formula, 0.3≦(Rxe/Rxc)≦0.75, more preferably, formulas, 0.3≦(Rxe/Rxc)≦0.5, 4.5≦(Rxc/USD)≦8.5, 0.3≦(Rye/Ryc)≦1.0, and Rxe≦Rde≦Rye. Also, the USD, a diagonal size of an effective surface of the panel is 500 mm or less than, a transmission ratio of the center portion of the panel is 45%˜75%, and the wedge ratio of 180%˜220% is satisfied.
Also, in case of using the invar mask and increasing the wedge ratio as 200% or more than, the super arc ratio is 22%˜24% and the inner curvature radius satisfies following formulas, 0.3≦(Rxe/Rxc)≦0.75, more preferably, formulas, 0.5≦(Rxe/Rxc)≦0.75 and 4.5≦(Rxc/USD)≦6.5.
As shown, a super arc ratio along a short axis can be expressed as 0.3≦(Rye/Ryc)≦1.0 as a relation formula of the curvature radius.
When the Rye/Ryc is 0.3 or more than, the drop characteristic of the cathode ray tube is satisfied. The Rye/Ryc shows a maximum value at 0.45 and is gradually decreased. In case that the Rye/Ryc is 1.0 or more than, the drop characteristic of the cathode ray tube is scarcely satisfied.
For reference, a measuring point of the partial doming is positioned on the longer side, so that the partial doming is influenced only by the long axis not by the short axis. On the contrary, the drop characteristic is influenced by both the long axis and the short axis.
As shown, the drop characteristic is satisfied even in the invar mask when the wedge ratio is 230% or more than. Therefore, in case of applying mask of material having a high intensity, ultra invar mask, or super invar mask besides the currently used invar mask, a structural intensity of the mask is increased thus to satisfy a formula, 0.3≦(Rxe/Rxc)≦0.75 in the wedge ratio of 210% or less than.
Also, in case of using a mask of another material having a middle thermal expansion coefficient between the invar material and the AK material, the partial doming is decreased thus to satisfy a formula, 0.3≦(Rxe/Rxc)≦0.75.
In the method for reducing the partial doming by the super arc, the Rxe, the inner curvature radius at an edge of the long axis is the smallest and the Rye, the inner curvature radius at an edge of the short axis is the greatest, which can be expressed as Rxe≦Rde≦Rye.
In the present invention, the super arc ratio is gradually increased towards the long axis in order to form a curvature at a ⅓ point of the long axis, a measuring point of the partial doming greatly. Therefore, the inner curvature of the edge of the effective surface along the long axis is relatively formed to be greater than that along the short axis or that along the diagonal axis.
The present invention is more effective in a cathode ray tube of 21″ or less than of which USD is 500 mm or less than. Also, in case of a large cathode ray tube, since the large cathode ray tube requires lower drop characteristic G than a smaller cathode ray tube, the present invention can be also applied to the large cathode ray tube.
As aforementioned, at the time of forming the inner curvature of the panel according to the present invention, relations among the inner curvature radius at a center of a long axis of the panel (Rxc), the inner curvature radius at an edge of a long axis of the panel (Rxe), the inner curvature radius at a center of a short axis of the panel (Ryc), the inner curvature radius at an edge of a short axis of the panel (Rye), the inner curvature radius at an edge of the diagonal axis of the panel (Rde), and the diagonal size of an effective surface of the panel (USD) are set, and the inner curvature of the panel is increased from the center portion of the panel towards the peripheral portion of the effective surface, thereby obtaining a structural intensity of the mask, thus increasing the drop characteristic, and effectively preventing the partial doming.
As the present invention may be embodied in several forms without departing from the spirit or essential characteristics thereof, it should also be understood that the above-described embodiments are not limited by any of the details of the foregoing description, unless otherwise specified, but rather should be construed broadly within its spirit and scope as defined in the appended claims, and therefore all changes and modifications that fall within the metes and bounds of the claims, or equivalence of such metes and bounds are therefore intended to be embraced by the appended claims.
| Number | Date | Country | Kind |
|---|---|---|---|
| 10-2003-0041730 | Jun 2003 | KR | national |
| Number | Name | Date | Kind |
|---|---|---|---|
| 4623818 | Yamazaki | Nov 1986 | A |
| 5416379 | Inoue et al. | May 1995 | A |
| 5519283 | Opresko et al. | May 1996 | A |
| Number | Date | Country | |
|---|---|---|---|
| 20040263054 A1 | Dec 2004 | US |
