US3902145A

US3902145A - Magnetic correction device for a cathode ray tube

Info

Publication number: US3902145A
Application number: US457562A
Authority: US
Inventors: Antonie Slavenburg; Den Boogert Johannes Van; Antoon Swart
Original assignee: US Philips Corp
Current assignee: US Philips Corp
Priority date: 1973-04-09
Filing date: 1974-04-03
Publication date: 1975-08-26
Anticipated expiration: 1992-08-26
Also published as: CA993028A; BE813434A; NL7304887A; ES425065A1; JPS5012964A; GB1466732A; DE2416509B2; AU6767074A; FR2224869B1; ZA742104B; BR7402789D0; DE2416509C3; NL160426B; DE2416509A1; NL160426C; IT1011709B; FR2224869A1; SE386008B; JPS5531985B2

Abstract

Magnetic correction device for a cathode ray tube, which device comprises a plurality of ring pairs which are secured to supports and each consist of rings which have magnetic poles distributed about their peripheries. The two rings of each pair are concentrically mounted and preferably are interconnected by a pinion so as to be rotatable in opposite senses.

Description

United States Patent 11 1 Slavenburg et al.

[ Aug. 26, 1975 1 MAGNETIC CORRECTION DEVICE FOR A CATIIODE RAY TUBE [75] Inventors: Antonie Slavenburg; Johannes van den Boogert; Antoon Swart, all of Emmasingel Eindhoven.

Netherlands [73] Assignee: U.S. Philips Corporation, New

York N.Y.

[22] Filed: Apr. 3, I974 1211 Appl. 1961457562 [30] Foreign Application Priority Data Apr. 9 1973 Netherlands 7304887 [52] U.S. CI 2 335/212; 335/210 [51] Int. Cl. 3 H0lf 7/00 [58] Field of Search 335/212. 210

[56] References Cited UNITED STATES PATENTS Loughrcn 335/2l2 2525919 ill/I950 2.801.356 7 1957 Hcppner 335/212 3332.046 7/1967 MCIOIIC 335/212 3341729 9 1967 Suari 11 335/212 3605053 9/1971 Anthony. 335/212 R27,698 7/1973 Werst .1 335 212 Primary hlumrimr-Hurold Broomc Attorney, Agenl, 0r FirmFrank R. Trifari; Henry I. Stcckler I57] ABSTRACT Magnetic correction device for a cathode ray tube, which device comprises a plurality of ring pairs which are secured to supports and each consist of rings which have magnetic poles distributed about their peripheries. The two rings of each pair are concentrically mounted and preferably are interconnected by a pinion so as to be rotatable in opposite senses.

I3 Claims 11 Drawing Figures MAGNETIC CORRECTION DEVICE FOR A CATHODE RAY TUBE The invention relates to a magnetic correction device for influencing the paths of electron beams produced in a cathode ray tube, which device comprises at least one support made of a non-magnetic material, securing means for securing the support on the neck of a cathode ray tube, and at least one pair of coaxial rings hav ing magnetic poles distributed about their peripheries, which rings are mounted on the support and are rotatable about their axes in opposite relative directions.

Such correction devices are used, for example, in colour television display tubes for correcting the paths of the electron beams so that firstly each beam impinges on only that part of a phosphor pattern provided on the display screen of the tube which luminesces in the correct colour (colour purity) and secondly the three beams intersect at the correct location (convergence). Such a device is described, for example, in re-issued US. Pat. No. Re. 27,209. A present trend in the design of television receivers is to reduce the receiver depth to a minimum. This depth is substantially exclusively determined by the length of the display tube, one of the factors which govern this length being the axial dimen sions of the correction device. Hence it is desirable for this dimension to be as small as possible.

It is an object of the present invention to provide a construction which satisfies this requirement. For this purpose the device according to the invention is characterized in that one of the two rings of a pair has an inner diameter which is greater than the outer diameter of the other ring, the smaller ring being mounted within the larger ring, whilst the outer ring has teeth on its inner periphery and the inner ring has teeth on its outer periphery, at least one pinion which is rotatable about a spindle secured to the support and extending parallel to the axis of the ring pair being located in the space between the two rings and meshing with the said teeth. Preferably the two rings have equal numbers of teeth, causing them to rotate through equal and opposite angles.

For the purpose of corrective adjustment the rings and/or the support preferably have lugs which radially project to the exterior.

An embodiment which enables the correction device to be readily mounted on the tube neck and the support to be readily rotated for adjusting the desired correction is characterized in that the securing means for securing the support on the neck of a cathode ray tube comprise an intermediate ring which is adapted to be coaxially mounted on the tube neck and to which at least one support is secured so as to be rotatable about the intermediate ring as a spindle.

An embodiment of the invention will now be described by way of example with reference to the accompanying diagrammatic drawings, in which:

FIG. 1 is a schematic side elevation of a cathode ray tube provided with a correction device according to the invention,

FIGS. 2a to 2(' illustrate the corrections to be effected by means of the correction device according to the invention.

FIG. 3 is a front elevation of a support which carries a pair of rings and forms part of the correction device according to the invention.

FIG. 4 is a longitudinal sectional view of the support and the ring pair shown in FIG. 3,

FIG. 5 is an exploded perspective view of the correction device according to the invention,

FIG. 6 is a side elevation of the correction device shown in FIG. 5,

FIG. 7 is a developed view of a portion of the thrust ring which forms part of the device shown in FIGS. 5 and 6, and

FIGS. 8a and 8b are a longitudinal sectional view and a cross-sectional view respectively of an extension for use with the device shown in FIGS. 5 and 6.

Referring now to FIG. 1, there is schematically shown a cathode ray tube which comprises a cylindrical neck 1 and a flaring part 3 which at the front carries a display screen 5. The neck contains three electron guns 7 which are arranged side by side, only one of them being shown (in broken lines), and are capable of producing three electron beams which extend side by side in a horizontal plane. A known deflection system 9 is provided for deflecting the said electron beams so that they scan the entire display screen 5, which system surrounds the tube at the junction of the neck 1 and the flaring part 3. A magnetic correcting device 11 is mounted on the tube neck for correcting directional errors of the three electron beams produced by the electron guns 7. The corrections to be performed by means of such a device are illustrated in FIGS. 2a to 20. In these Figures the three electron beams are designated 13, 15 and 17 respectively. The display screen 5 is provided with a pattern of vertical stripes of phosphor which when struck by an electron beam luminesce in one of the colours red, green and blue (not shown). A colour selection electrode (shadow mask) 19 (shown in broken lines in FIG. 1) serves to ensure that each electron beam can impinge on phosphor stripes of one colour only. The beam 13 is to strike the red phosphor, the beam 15 the green phosphor, and the beam 17 the blue phosphor. Owing to inevitable inaccuracies in manufacturing the tube and the deflection system deviations from the ideal situation are found to occur in practice. These deviations will be readily apparent when a grid of horizontal and vertical white lines is dis played on the display screen 5. In actual fact such a grid comprises three exactly registering grids of red, green and blue lines respectively. The first error which may occur consists in that the electron beams do not always impinge on the phosphor stripes of the correct colour only, i.e. part of, for example, the green beam may strike the green phosphor and part may strike the red phosphor. This error can be corrected by shifting the beams in a horizontal direction, for example by producing a magnetic field the lines of force of which extend in the vertical direction at the location of the beams, i.e. centrally of the tube neck 1. This may be effected. for example in the manner shown in FIG. 2a, by means of a magnetic ring 21 having two diametrically opposed magnetic poles. Magnetic lines of force 23 cause horizontal shifting of the beam 15 (and also of the beams 13 and 17) in the direction indicated by arrows 25. The strength of the magnetic field and hence the magnitude of the shift 25 can be rendered controllable by rotating two rings 21 in opposite directions (this step is known). Rotation of both rings through enables the shift to be varied from extreme right via zero to extreme left. This correction is referred to as colour purity correction.

A second possible error is that the three grids (which after the colour purity correction each have the correct colour) are not in register. This error (convergence error) can be corrected in two steps. First (see FIG. 2b) the red and blue grids are made to register by shifting the

beams

13 and 17 in opposite directions. For this purpose a quadrupolar magnetic field is produced (in known manner) by means of a magnetic ring 27 which has four poles distributed about its periphery. At the locations of the

beams

13 and 17 lines of force 29 of the magnetic field produced by the ring 27 always extend in opposite directions so that shifts 31 and 33 of said beams also have opposite directions. The strength of the quadrupolar field can be controlled, in the same manner as that of the bipolar field of the colour purity ring 21, by rotating two rings 27 in opposite directions. The directions of the

shifts

21 and 33 can be controlled by jointly rotating the two rings 27 in the same direction. FIG. 2b shows further that the ring 27 does not produce a magnetic field at the location of the middle beam and hence this beam is not influenced.

After the red and blue grids have been superimposed on one another in the manner described, the resulting combined grid must be brought into register with the green grid. For this purpose the

beams

13 and 17 are to be shifted in the same direction through equal distances, as is shown in FIG. 20. This can be obtained by means of a sextupolar magnetic field which is produced by a magnetic ring 35 having six magnetic poles distributed about its periphery. As FIG. shows, magnetic lines of force 37 then have the same direction at the locations of the

beams

13 and 17, so that the

shifts

39 and 41 respectively of these beams are identical. In complete analogy with the situation illustrated by FIG. 2b the magnitude and the direction of the shifts are adjustable by rotating the two rings 35 first in opposite senses and then in the same sense. In this case also, the resulting magnetic field strength at the location of the green beam 15 is zero.

From the above it will be obvious that for each possibility of correction a pair of rings having magnetic poles distributed about their peripheries are required which are to be rotatable in opposite senses and, in many cases, jointly in the same sense also. To enable the axial length of the correction device 11 yet to be re duced to a minimum pairs of

rings

43, 45 are designed so that one of the rings (43) has an inner diameter which is greater than the outer diameter of the other ring (45). As FIGS. 3 and 4 show, the smaller ring 45 is mounted concentrically within the larger ring 43. The two rings 43 and 45 are disposed on a likewise ring-shaped support 47 which can be mounted on the tube neck so as to be rotatable together with the ring pair about the axis of the tube. The support 47 has a protruding rim 48 along its inner circumference for the purpose of centering the ring pair. In order to enable the two rings 43 and 45-to be rotated in opposite directions also, preferably the outer ring 43 is provided with teeth 49 along its inner periphery whilst the inner ring 45 is provided with teeth 51 along its outer periphery. In the space between the two rings 43 and 45 a pinion 53 is mounted which meshes with both sets of

teeth

49 and 51. The pinion 53 is arranged to revolve about a spindle 55 formed on the support 47 and extending par allel to the axis of the ring pair. In order to drive the two

rings

43 and 45 the outer ring 43 only has to be rotated, the inner ring 45 then being automatically rotated in the opposite sense. For this purpose the outer ring 43 is provided with radially projecting lugs 57, four in the present embodiment. Adjustment of the magnetic field strength will be easiest if the two

rings

43 and 45 always rotate in opposite senses through equal angles. This is obtained by using equal numbers of

teeth

49 and 51. If desired, two or more pinions 53 may be used which may be distributed about the space between the two

rings

43 and 45. In order to facilitate rotation of the support 47 this also is provided with a number of radially projecting lugs 59 (one in the present case).

A correction device comprising three supports 47 each carrying a

ring pair

43, 45 is shown in an exploded perspective view in FIG. 5 and in side elevation in FIG. 6. The three supports 47 are secured one behind the other to an intermediate ring 61 having an inner diameter such as to fit around the tube neck with a small amount of clearance. In order to enable the intermediate ring 61 to be clamped to the tube neck its inner diameter increases towards one end (the righthand end in FIG. 5; this increase is not visible in the drawings), a conical clamping ring 63 fitting within this end. The conical clamping rings 63 has a gap 64 which progressively closes as the ring is axially thrust into the flaring part of the intermediate ring 63. As a result the diameter of the conical clamping ring 63 is decreased so that it firmly encloses the tube neck. To increase the friction between clamping ring 63 and the glass of the tube neck 1 the ring is internally provided with rubber strips 65. To enable axial pressure to be exerted on the clamping ring 63 a ring 67 is provided which by means of radial inward projections 69 engages behind a collar 71 formed on the intermediate ring 61 and has inclined rim sections 73 which cooperate with inclined rim sections 75 of the conical clamping ring 63, so that rotation of the ring 67 results in axial displacement of the clamping ring 63. To facilitate rotation of the ring 67 it is provided with a radially protruding lug 77.

The outer diameter of the intermediate ring 61 is such that it fits with a small amount of clearance in the support 47 and hence can be used as a spindle for rotation of the supports. As has been set out with reference to FIG. 2a, the colour purity correction may in some cases be effected by causing two diametrically magnetised rings to revolve in opposite senses without the need for joint rotation. In this case the support 47 for the colour purity rings may be locked against rotation about the intermediate ring, which may have advantages, as will be set forth hereinafter. For efficient manufacture of the support 47 it is desirable to use supports of a single type only which are capable of being mounted on the intermediate ring 61 so as to be either rotatable or locked. For this purpose the protruding rim 48 along the inner periphery of the support 47 is formed with one or more gaps 79, a corresponding number of projections 81 being formed on the intermediate ring 61. When a support 47 is placed on the intermediate ring 61 so that a projection 81 is received in a gap 79, the support is locked against rotation. The supports 47 which are mounted in front of or behind the projections 81 are freely rotatable. In the embodiment shown in FIGS. 5 and 6 the middle support 47 (which carries diametrically magnetised rings 43 and 45) is locked and is flanked on either side by a rotatable support. One of these rotatable supports carries rings 43 and 45 which each have four magnetic poles distributed about their peripheries for effecting the correction described with reference to FIG. 2b, the other rotatable support carrying rings which each have six poles distributed about their peripheries for performing the correction described with reference to FIG. 20. Because the locked support is interposed between the two rotatable supports, rotation of one of the rotatable supports is prevented from being transmitted to the other by friction.

Thus the rotary movements of the rotatable supports are entirely independent of one another. To prevent a corrected condition from being incidentally upset, preferably means are provided to lock the supports and possibly the rings against further rotation around the intermediate ring. For this purpose each support 47 is provided on its major surfaces with knurled areas 83 located on raised portions which also serve to center the outer ring 43. When the set of supports 47 is axially compressed, the said knurled areas ensure mutual locking. Because the middle support is locked against rotation by the projection 81, the outer supports also are locked against rotation. Axial compression of the set of supports is performed by means of a thrust ring 85 mounted for rotation around the intermediate ring 61. This thrust ring near its inner periphery has a portion 87 the thickness of which varies the peripheral direction. FIG. 7 shows the developed portion 87. This portion is located between a radial projection 89 formed on the intermediate ring 61 and the left-hand support 47. The various component parts are proportioned so that the projection 89 and the left-hand support 47 are spaced from one another by a distance intermediate between the smallest thickness x and the largest thickness y of the portion 87 of the thrust ring 85. Thus on rotation of the thrust ring 85 the portion 87 acts as a wedge which axially clamps the central supports. To facilitate the said rotation the thrust ring 85 is provided with radially projecting lugs 91. To prevent undue rotation of the thrust ring 85 the portion 87 has a knurled surface 92. In the embodiment shown the support 47 only can be locked against rotation. Obviously the rings 43 and- /or 45 may also be provided with knurled areas which can engage corresponding knurled areas on the support 47, enabling the said rings also to be locked. Other locking means may be used, for example a braking block adapted to be forced against the rims of the supports 47 and the outer rings 43, which block and which rims may also be knurled.

When the

lugs

57 and 59 of the rings 43 and the support 47 respectively are in substantially equal angular positions, it may be difficult to move one lug by hand without unintentionally moving the other. Hence the said lugs preferably are adapted to be axially extended for example by means of a simple extension 93 which is shown in FIG. 8 and comprises a cavity 95 adapted to be slipped onto the

lugs

57, 59 and a handle 97.

In the embodiment described the correction device comprises three supports carrying ring pairs for effecting the corrections described with reference to FIG. 2. Obviously, if desired, a higher or lower number of supports may be used and furthermore the number of magnetic poles of each ring and their distribution about the periphery of each ring may be matched to the respective requirements. Thus, the correction device according to the invention is suitable for solving many different correction problems, also in cathode ray tubes of types different from that shown in FIG. 1 having three electron guns arranged side by side.

For manufacturing the correction device, as far as possible material of low magnetic permeability, for ex ample a synthetic material, is used to prevent the stray field at the rear of the deflection system 9 from influ encing the electron beams via the correction device. This also applies to the

rings

43, 45, which may be made of a low-permeability magnetic material, as is the case in the embodiment described, or of a synthetic material, in which case magnets of locally secured to them, for example by means of an adhesive.

What is claimed is:

1. Magnetic correction device for influencing the paths of electron beams produced in a cathode ray tube, which device comprises at least one support made of a non-magnetic material, securing means for securing the support to the neck of a cathode ray tube, and at least one pair of coaxial rings having magnetic poles distributed about their peripheries, which rings are mounted on the support and are rotatable about their axes in opposite relative directions, characterized in that one of the two rings of a pair has an inner diameter which is greater than the outer diameter of the other ring, the smaller ring being mounted within the larger ring, whilst the outer ring has teeth on its inner periphery and the inner ring has teeth on its outer periphery, at least one pinion, which is rotatable about a spindle secured to the support and extending parallel to the axis of the ring pair, being located in the space between the two rings and meshing with the said teeth.

2. Correction device as claimed in claim 1, character ized in that the teeth on the two rings are equal in numher.

3. Correction device as claimed in claim 1, characterized in that the outer ring is provided with at least one radially externally projecting lug.

4. Correction device as claimed in claim 3, characterized in that the support also is provided with at least one radial lug which projects to the exterior.

5. Correction device as claimed in claim 3, characterized in that the lugs are radially extensible by means of an extension adapted to be slipped on one of the lugs.

6. Correction device as claimed in claim 1, characterized in that the securing means for securing the support to the neck of a cathode ray tube comprise an intermediate ring which is adapted to be coaxially placed around the tube neck and to which at least one support is secured so as to be rotatable about the intermediate ring as a spindle.

7. Correction device as claimed in claim 6, characterized in that two supports are provided which are spacedly and axially rotatably secured to the intermediate ring, each of the rings carried by the first support having four magnetic poles distributed about its periphery, whilst each of the rings carried by the second support has six magnetic poles distributed about its periphery.

8. Correction device as claimed in claim 7, characterized in that between the two supports which are rotatably secured to the intermediate ring a third support is secured to the intermediate ring so as to be locked against rotation, each of the rings carried by the third support having two diametrically arranged magnetic poles.

9. Correction device as claimed in claim 6, characterizedjn that means are provided for locking each sup port against rotation about the intermediate ring after the desired correction has been effected.

l0. Correction device as claimed in claim 9, characterized in that the locking means comprise knurled areas which are provided on each rotatable supports (47) and are capable of engaging a knurled area which is not rotatable relative to the intermediate ring.

11. Correction device as claimed in claim 10, characterized in that the knurled areas are located on the major surfaces of each support and the non-rotatable knurled area is located on the middle, non-rotatable support, thrust means being provided for exerting an axial force on the set of supports.

12. Correction device as claimed in claim 11, characterized in that the thrust means comprise a thrust ring which is secured to the intermediate ring and is rotatable about'the intermediate ring as a spindle and the thickness of which varies in the peripheral direction at least near the inner periphery, the portion of varying thickness being located between at least one radial projection formed on the intermediate ring and one of the

Claims

2. Correction device as claimed in claim 1, characterized in that the teeth on the two rings are equal in number.

9. Correction device as claimed in claim 6, characterized in that means are provided for locking each support against rotation about the intermediate ring after the desired correction has been effected.

10. Correction device as claimed in claim 9, characterized in that the locking means comprise knurled areas which are provided on each rotatable supports (47) and are capable of engaging a knurled area which is not rotatable relative to the intermediate ring.

12. Correction device as claimed in claim 11, characterized in that the thrust means comprise a thrust ring which is secured to the intermediate ring and is rotatable about the intermediate ring as a spindle and the thickness of which varies in the peripheral direction at least near the inner periphery, the portion of varying thickness being located between at least one radial projection formed on the intermediate ring and one of the supports, the arrangement being such that the spacing between the projection and the said support is greater than the smallest thickness and smaller than the greatest thickness of the said portion of the thrust ring.

13. Correction device as claimed in claim 6, characterized in that a conical clamping ring is provided to secure the intermediate ring to the neck of a cathode ray tube.