EP0095617B1 - Tube-image couleurs comprenant des moyens de correction des défauts de torsion - Google Patents
Tube-image couleurs comprenant des moyens de correction des défauts de torsion Download PDFInfo
- Publication number
- EP0095617B1 EP0095617B1 EP83104638A EP83104638A EP0095617B1 EP 0095617 B1 EP0095617 B1 EP 0095617B1 EP 83104638 A EP83104638 A EP 83104638A EP 83104638 A EP83104638 A EP 83104638A EP 0095617 B1 EP0095617 B1 EP 0095617B1
- Authority
- EP
- European Patent Office
- Prior art keywords
- correction
- electron
- magnets
- magnet
- picture tube
- 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
- 238000010894 electron beam technology Methods 0.000 claims description 53
- 230000005415 magnetization Effects 0.000 claims description 17
- 238000004519 manufacturing process Methods 0.000 description 8
- 230000000694 effects Effects 0.000 description 3
- 230000003068 static effect Effects 0.000 description 3
- 238000006073 displacement reaction Methods 0.000 description 2
- 238000010276 construction Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
Images
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
- H01J29/46—Arrangements of electrodes and associated parts for generating or controlling the ray or beam, e.g. electron-optical arrangement
- H01J29/70—Arrangements for deflecting ray or beam
- H01J29/701—Systems for correcting deviation or convergence of a plurality of beams by means of magnetic fields at least
- H01J29/702—Convergence correction arrangements therefor
- H01J29/703—Static convergence systems
-
- 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
- H01J29/46—Arrangements of electrodes and associated parts for generating or controlling the ray or beam, e.g. electron-optical arrangement
- H01J29/48—Electron guns
- H01J29/51—Arrangements for controlling convergence of a plurality of beams by means of electric field only
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J2229/00—Details of cathode ray tubes or electron beam tubes
- H01J2229/58—Electron beam control inside the vessel
- H01J2229/581—Electron beam control inside the vessel by magnetic means
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J2229/00—Details of cathode ray tubes or electron beam tubes
- H01J2229/58—Electron beam control inside the vessel
- H01J2229/583—Electron beam control inside the vessel at the source
- H01J2229/5835—Electron beam control inside the vessel at the source cooperating with the electron gun
Definitions
- the invention relates to a color picture tube consisting of a screen trough, cone and neck, in which the screen trough is provided with a fluorescent screen and mask and an inline electron gun system with at least one correction magnet is arranged in the neck.
- the screen image is produced by horizontal and vertical deflection of three electron beams which meet in the plane of the mask provided with openings, the electron beams passing through the openings in different directions and the ones assigned to them, arranged on the one behind the mask Excite the fluorescent screen adjacent fluorescent areas.
- the static convergence of the color picture tube is set when the three electron beams run without a deflection field in such a way that they hit the center of the mask together.
- Static color purity is present when the electron beams hit the fluorescent areas of the fluorescent screen assigned to them through the openings in the mask at the correct angle. Dynamic convergence and color purity are maintained if color purity and convergence are present on the entire fluorescent screen when the electron beams are deflected together by the magnetic field of the deflection unit.
- a ring made of easily magnetizable permanent magnet material, which is located at the level of the grating 3 above the electron gun system.
- a further magnetizable wire ring can be arranged alone or additionally on the end of the electron gun system facing the fluorescent screen. This wire ring can also be present in the convergence electrode.
- the rings are magnetized on their circumference so multipolar that the electron beams experience the necessary corrective deflections.
- twist error which consists in that the lines written by the three electron beams when deflected on the screen are inclined towards one another with the aid of the multipolar magnetized ring mentioned above, does not succeed because at the same time with the reduction of the Twist error other dynamic errors arise.
- This is very disadvantageous because it is therefore not possible to effectively eliminate the twist error, so that color picture tubes with such construction errors have to be reworked in such a way that a new electron gun system is used.
- the object of the invention is to provide an inexpensive device for correcting twist errors.
- Claims 2 to 5 indicate advantageous refinements of the invention.
- the electron beams to be corrected are deflected by additional correction magnets before entering the magnetic field of the deflection unit and before passing through the correction fields for color purity and convergence.
- correction magnets are attached near the external electron beams and magnetized in such a way that the electron beams can be deflected in different directions, that is, from the plane in which the three electron beam generator systems lie.
- the central electron beam should not be influenced by the correction magnets.
- the magnetization of the correction magnets in color picture tube production can take place on the same machine on which other correction magnets are also set.
- a ring of magnetizing coils with strongly bundled magnetic fields is arranged displaceably in the direction of the longitudinal axis of the color picture tube in place of the correction magnets to be magnetized.
- the effect of the magnetizations is measured with the aid of sensors arranged in front of the luminescent screen, and the magnetization of the correction magnets then continues until they have the required magnetization.
- the color picture tube in Figure 1 consists of the screen trough 7 with the fluorescent screen 1 and the mask 2, the cone 6 and the neck 5 and has the electron gun system 3, which is located in the neck 5 of the color picture tube.
- the electron gun system is shown enlarged in Figure 2. It has a correction magnet 10 for the correction of color purity and convergence and a correction magnet 11 which makes this correction free of twist errors.
- FIG. 3 shows in dashed lines the course of an electron beam that is only convergent-corrected with a correction magnet 10 and requires correction and dash-dot lines the course of an electron beam corrected for convergence with two correction magnets 10 and 11 without twist errors.
- the curve shown in dashed lines arises when a correction magnet 10 is present.
- the dash-dotted curve occurs when the correction magnet 11 is arranged in addition to the correction magnet 10.
- the course of an electron beam not requiring correction up to the correction magnet 10 is shown in dotted lines. Both the courses of the electron beam shown in FIG. 3, starting from the cathode 24, end on the center of the luminescent screen 14.
- the convergence correction is carried out with the correction magnet 10 arranged at the level of the line 12.
- the twist error-free convergence correction is prepared by a further correction magnet 11, which corrects itself in the amount of Line 13 is located.
- FIG. 4 shows how the deflection takes place without the correction magnets 11.
- FIG. 5 shows how the correction magnets 11 according to the invention, which lie in a plane containing the section line 13, direct the course of an electron beam, which is initially shown in broken lines, toward the plane 19.
- the deflection of the electron beam into the plane 19 is effected by the correction magnet 10, which is located in the plane containing the section line 12.
- the corrected electron beam then runs on the now correct, dash-dotted path into the magnetic field of the deflection unit and thus does not cause any dynamic distortions during the deflection.
- the dashed line corresponds to the course of an electron beam corrected only by a correction magnet 10.
- the dotted line corresponds to the course of an electron beam that does not require correction.
- Figure 6 shows an embodiment for the arrangement and design of the correction magnets 11.
- the openings 20 through which the outer electron beams enter the grid 3 lie in the area of influence of the correction magnets 11, which can be shaped in an I, U or E shape. They are preferably fixed in the part 21 of the grid 3 of the electron gun system facing the cathode in a non-positive or positive manner.
- the correction magnets 10 are provided in the middle part 22 of the grating 3.
- FIG. 7 an embodiment with U-shaped correction magnet 11 is shown, in Fig. 8 with an E-shaped correction magnet.
- the correction magnets 11 can also be attached to the outside of the grating 3.
- a corresponding arrangement on the grid 2, inside or outside, is also possible.
- FIG. 10 gives an example of the closely adjacent attachment of correction magnets 10 inside the grid 3 in the form of clips and the correction magnets 11 outside on the grid 3 as a U-shaped bracket.
- the shape of the correction magnets can be seen from FIGS. 11 and 12: FIG. 11 is the section AB in FIG. 10 and FIG. 12 shows the section CD of FIG. 10.
- FIG. 13 is a representation of a structure with correction magnet 10 in two planes and a correction magnet 11 in one plane.
- section AB of FIG. 13 which is shown in FIG. 14, correction magnets 10 divided by air gaps are inserted into the central part of the grating 3, while in FIG. 15 section CD of FIG. 13 shows I-shaped correction magnets 11 which two basic forms of magnetization are symbolically illustrated.
- the magnetization with three magnetic poles shown on the left effects the displacement of the electron beam perpendicular to the plane of the electron beams, while the magnetization with two magnetic poles indicated on the right in FIG. 15 causes a deflection of the neighboring electron beam in a horizontal direction.
- one or both of the outer electron gun systems may twist from the intended plane.
- the deflection unit is aligned precisely with the horizontal desired position of this plane, so that twisted electron beams with positional deviations enter the magnetic field of the deflection unit.
- a twist angle a results, which leads to dynamic convergence errors.
- the twist error is eliminated by the magnetization of the correction magnet 11 according to the invention alternating with the magnetization of the correction magnet 10.
- the dosing of the twist correction is done by the different magnetization of the correction magnets. If the electron beam path is influenced in this way, this path is bent twice. This not only corrects the direction of the course, but also the position of the electron beam.
- a simultaneous correction of the course of the two outer electron beams is possible and desirable, but is not absolutely necessary because of the already satisfactory effect in the case of asymmetrical correction. It can be sufficient to influence an external beam, i. H. the correspondingly dimensioned two-pole field of a correction magnet 11 with a suitable arrangement for the electron beam is sufficient.
- correction magnet (s) 11 are arranged in the beam generator system, e.g. Correction magnets 11 used in the form of pieces of wire, which are preferably attached to the bottom of the inner edge of grid 3.
- the magnetization coils that are already present for the magnetization of the correction magnets 10 can be used to magnetize the wire pieces, which are temporarily brought to the height of the correction magnets 11 on the electron gun system.
- magnet bundles provided with one or more air gaps can also be used if the magnetizing coils can be used to achieve a narrowly delimited, that is to say sharply localized magnetization of the magnetic stirrups near the outside beams.
- Pieces of wire or brackets are attached to the grid 3 in a non-positive or positive manner on the inside or outside.
- the shape of the correction magnets and their geometric position on the longitudinal axis of the electron gun system depends on the properties of the type of color picture tube concerned and can also differ from the exemplary embodiment shown in FIG. 6. So correction magnets 11 z. B. are also in the upper part 23 of the grid 3 when the correction magnets 10 are in the grid 4, the so-called convergence pot.
- correction magnets 11 are low, so that all color picture tubes can be equipped with the correction magnets 11 during their manufacture. In this way, more than half of the rejects caused by twist errors, which would make it necessary to re-glaze an electron gun system, can be avoided.
- the magnetization of the correction magnets 11 must take place in such a way that the magnetic field of the correction magnet influencing the adjacent external beam runs in the plane of the electron beams.
- the magnetic field of the correction magnet at the location of the electron beam then shifts it out of the plane, as illustrated on the left in FIG. 15.
- Magnetizing the correction magnet, as indicated on the right in FIG. 15 creates a magnetic field perpendicular to the plane of the electron beams at the location of the adjacent external beam.
- the resulting displacement of the relevant outside beam thus takes place in the plane of the Electron beams, which then also supports the color purity and convergence correction.
- the electron beam is displaced in any direction, so that deflection of the outer electron beams can be achieved in all directions between vertical and horizontal.
Landscapes
- Video Image Reproduction Devices For Color Tv Systems (AREA)
- Agricultural Chemicals And Associated Chemicals (AREA)
Claims (5)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE3219954 | 1982-05-27 | ||
DE19823219954 DE3219954A1 (de) | 1982-05-27 | 1982-05-27 | Farbbildroehre mit twistkorrektur |
Publications (3)
Publication Number | Publication Date |
---|---|
EP0095617A2 EP0095617A2 (fr) | 1983-12-07 |
EP0095617A3 EP0095617A3 (en) | 1984-10-17 |
EP0095617B1 true EP0095617B1 (fr) | 1987-11-19 |
Family
ID=6164634
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP83104638A Expired EP0095617B1 (fr) | 1982-05-27 | 1983-05-11 | Tube-image couleurs comprenant des moyens de correction des défauts de torsion |
Country Status (5)
Country | Link |
---|---|
US (1) | US4625144A (fr) |
EP (1) | EP0095617B1 (fr) |
JP (1) | JPS58218732A (fr) |
CA (2) | CA1206321A (fr) |
DE (2) | DE3219954A1 (fr) |
Families Citing this family (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2728212B2 (ja) * | 1988-11-22 | 1998-03-18 | 株式会社日立製作所 | カラーブラウン管装置 |
US5233267A (en) * | 1989-10-03 | 1993-08-03 | Matsushita Electronics Corporation | Dynamic convergence system for color cathode ray tubes having an in line electron gun |
JP2945688B2 (ja) * | 1989-10-03 | 1999-09-06 | 松下電子工業株式会社 | カラー受像管装置 |
JP3135421B2 (ja) * | 1993-07-06 | 2001-02-13 | 松下電子工業株式会社 | カラー陰極線管 |
US5557164A (en) * | 1995-03-15 | 1996-09-17 | Chunghwa Picture Tubes, Ltd. | Cathode ray tube with misconvergence compensation |
KR100596229B1 (ko) * | 1998-09-29 | 2006-09-20 | 엘지전자 주식회사 | 컬러 음극선관 전자총 |
Family Cites Families (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3639796A (en) * | 1968-03-11 | 1972-02-01 | Sony Corp | Color convergence system having elongated magnets perpendicular to plane of plural beams |
FR2313832A1 (fr) * | 1975-06-06 | 1976-12-31 | Videon Sa | Procede et dispositif d'elimination des defauts de groupement des faisceaux electroniques dans un tube cathodique couleur a canons coplanaires |
DE2612607C3 (de) * | 1976-03-25 | 1984-01-12 | Philips Patentverwaltung Gmbh, 2000 Hamburg | Statische Konvergenzkorrekturvorrichtung in Farbfernsehbildwiedergaberöhren |
JPS5559637A (en) * | 1978-10-30 | 1980-05-06 | Hitachi Ltd | Magnetic focus cathode ray tube |
DE3003197A1 (de) * | 1980-01-30 | 1981-08-06 | Standard Elektrik Lorenz Ag, 7000 Stuttgart | Vorrichtung zum einstellen der elektronenstrahlen einer farbbildroehre |
GB2079530B (en) * | 1980-07-02 | 1985-04-11 | Hitachi Ltd | Magnetic focussing arrangement in a cathode ray tube |
-
1982
- 1982-05-27 DE DE19823219954 patent/DE3219954A1/de not_active Withdrawn
-
1983
- 1983-05-06 CA CA000427587A patent/CA1206321A/fr not_active Expired
- 1983-05-06 US US06/492,068 patent/US4625144A/en not_active Expired - Lifetime
- 1983-05-11 EP EP83104638A patent/EP0095617B1/fr not_active Expired
- 1983-05-11 DE DE8383104638T patent/DE3374625D1/de not_active Expired
- 1983-05-20 CA CA000428595A patent/CA1202059A/fr not_active Expired
- 1983-05-26 JP JP58093314A patent/JPS58218732A/ja active Pending
Also Published As
Publication number | Publication date |
---|---|
EP0095617A3 (en) | 1984-10-17 |
CA1202059A (fr) | 1986-03-18 |
EP0095617A2 (fr) | 1983-12-07 |
DE3219954A1 (de) | 1983-12-01 |
DE3374625D1 (en) | 1987-12-23 |
JPS58218732A (ja) | 1983-12-20 |
US4625144A (en) | 1986-11-25 |
CA1206321A (fr) | 1986-06-24 |
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