US2849647A

US2849647A - Color television reproducing device

Info

Publication number: US2849647A
Application number: US491163A
Authority: US
Inventors: Francken Jan Carel
Original assignee: US Philips Corp
Current assignee: US Philips Corp; North American Philips Co Inc
Priority date: 1954-03-04
Filing date: 1955-02-28
Publication date: 1958-08-26
Anticipated expiration: 1975-08-26

Description

Aug. 26, 1958 J. c. FRANCKEN COLOR TELEVISION REPRODUCING DEVICE Filed Feb. 28,1955

' 2 Sheets-Sheet 1 FIGJ.

INVENTOR JAN CAREL FRANCKEN Aug. 26, 1958 J. c. FRANCKEN I V COLOR TELEVISION REPRODUCING DEVICE Filed Feb. 28, 1955 2 Sheets-Sheet '2 FIG-.3

NVENTOR J. C. FRANCKBV CGLOR TELEVISION REPRODUCING DEVICE Jan Care! Francken, Emmasingel, Eindhoven, Netherlands, assignor, by mesne assignments, to North American Philips Company, Inc., New York, N. Y., a corporation of Delaware Application February 28-, 1955, Serial No. 491,163 Claims priority, application Netherlands March 4, 1954 6 Claims. (Cl. 315-13 images. Consequently, many suggestions have previously been made-for the construction of such tubes, in which the arrangement of the electrode systems for producing the, cathode rays, which systems: are referred to as electronguns, is dependent upon the way in which the images are-produced. One of the tubes most known comprises three electron guns, the axes of which are directed according to the edges of an equilateral prism. It has also been suggested to arrange the three guns in such manner that their axes extend in parallel and in one flat plane.

Tubes of the last-mentioned kind comprising three parallel guns are known for bothoscillography and reproducing colour television images. The object: of the firstkind of tubes is to-r-ecord simultaneously three oscillograms, so that it will be easily understood that each gun for this purpose comprises one or more deflection systems. In the above-mentioned tubes for colour. television comprising three guns locatedinone plane,each gun comprises a set of deflection electrodes of its own. The three sets of deflection electrodespermit of directing the three beams to one point on acollector. In the device concerned the collector or electron-receiving screen comprises a luminescent screen and a grid of parallel wires which is arranged in frontthereof and which produces an image of line structure. All three electron beams in this case are directed to the same area of the grid. In the description following hereinafter ofthe device according to the invention, the term collecting or electron-receiving screen must not be understoodto mean solely the-screen serving to produce the visibleimage. For certain systems the collectingor electron-receiving screen is actually only the luminescent screen, but for other systems the'collecting' or electron-receivingscreen is'a perforated electrode, for example a grid, arranged in frontof the luminescent screen. In the first-mentioned systems the three beams; are thus required 'to be directed tothe same point on the luminescent screen, whereas in the other systems it is more common practice to direct the beams to the same area of'the perforated electrode.

In the. above-mentioned colour television. tubes, comprising three guns, it is necessary for the three cathode rays to be directed to the same point on the collecting screen, even if the beams are deviated or scanned across the screen to produce a'raster-like image. This may be realized owing to each beam having a deflection or scanning system'of itsown, but it; is then necessary to apply deflection voltages of particular shape to the said systems. Said voltages are requiredtobe highly asymmetrical for writing a symmetrical raster:

A device according to the invention exhibits the abovementioned disadvantages to a greatly reduced extent and also affords some other advantages.

A device according to the invention for reproducing images, more particularly for reproducing colour television images, comprises a cathode-ray tube having three electron guns producing three electron rays or beams which scan a collecting screen under the action of a deviation or scanning field, common to all rays and comprising two relatively almost perpendicular components, which rays are always convergent upon leaving the three electron guns and which are located in a flat plane upon entering the deviation field. The device exhibits the characteristic that one component of the deviation or scanning field is parallel to the intersecting line of a plane at right angles to the axis of the tube and the plane of the cathode rays and is also characterized in that two out of the three electron guns each comprise an electrostatic deflecting system having applied to it voltages such that the meeting point of the three cathode rays is always locatedon the collecting screen.

The term deviation is to be understood inthis description to mean the common deviation or scanning of the three rays for producing the image raster. The term deflection is to be understood to mean the action exerted upon the electron rays to give themthe correct direction before entering the common deviation field.

' A device according to the invention affords the advantage that the deviation system may have applied to it simple voltages or currents of the usual shape, for example saw-tooth shape. Owing to the three electron rays, upon entering the deviation field, being located in one-plane, the advantage is obtained that, if for a determined intensity of the deviation field the rays meet at one point, such is always the case, apart from the error referred to as coma, even if the deviation is varied. When the three electron rays are regarded asparts of one beam, it can thus be said that any interfering astigmatism does not occur. However, one error still remains, viz. that the geometric position of the meeting point of the three rays is not a flat plane but falls along a curved surface. This constitutes a disadvantage, since the collecting screen can usually be regarded to a first approximation as a flat surface.

Since two electron guns comprise individual deflecting systems, it can primarily be ensured that the rays meet at one point on the collecting screen for a determined strength of the deviation field, and furthermore the necessary correcting voltages may be applied to the said defleeting systems, so that the above-mentioned curved surface is deformed so as to coincide with the collecting screen.

In a determined case it is even not necessary to aply voltages to the deflecting systems for bringing the three rays together at one point on the collecting screen, namely if the three electron guns are arranged at an angle to one another such that the axes of the guns already meet at one point on the collecting screen without voltages on deflecting systems. It is then only necessary to apply simple correcting voltages to the deflecting systems to ensure that the rays, when the deviation field is switched on, actually meet on the collecting screen.

Arranging the electron guns at an angle has a disadvantage, since in this case the space occupied by the electron guns is large with respect to the space occupied if the three guns are arranged with their axes in parallel. It is thus frequently more advantageous to arrange the three guns with their axes in parallel and to ensure by means of direct voltages on the deflecting systems that the three rays meet at a point on the collecting scree' when the deviation field is not switched. on.

It is naturally immaterial. which two out. of the three electron guns are provided with deflecting plates, since the direction of one electron ray may always be regarded as the correct direction, so that the other rays may be directed to the point at which the first-mentioned ray strikes the collecting screen.

If the axes of the three guns are located in parallel in a flat plane, it is very advantageous to provide the outer guns with deflecting plates, it then being possible to direct the central gun to the centre of the collecting screen. The whole structure of the electrode system is thus rendered symmetrical and hence simple.

Since the electron rays are located in a flat plane, they need be deflected only in this plane. If there should be small deviations bringing the rays outside this plane before reaching the deflection electrodes, they can be moved back into the plane by carrying out a correction with the use of magnets provided outside the tube. As before, the direction of one of the electron rays is usually regarded as the correct direction, the other two electron rays being deflected magnetically, so that all three rays come to lie in one plane. Preferably the two outer electron rays are thus influenced by magnetic means. However, in this case it is necessary for the central electron ray to be screened magnetically. This screening may consist, for example, of a ferromagnetic envelope surrounding at least part of the central gun. However, as an alternative, it is possible for one electrode of the central gun to be manufactured of ferromagnetic material.

In order that the invention may be readily carried into etfect, it will now be described with reference to the accompanying drawing, given by way of example, in which:

Fig. 1 shows a cross-sectional view of a cathode-ray device of the invention;

Figs. 2 and 3 orthogonal cross-sectional views of a modification. n i

In the figure, the cathode-ray tube comprises a cylindrical neck 1 and an adjoining conical portion 2, closed by a slightly curved window 3. The latter is covered on its inner side with a luminescent layer 4 serving as the electron-receiving screen. Arranged inside the neck 1 of the tube are three rectilinear parallel electron guns, the axes of which are located in one flat plane, i. e., the plane of the drawing. All three guns, except the deflection plates of the two outer ones, are identical, so that one gun only is provided with reference numerals for the sake of clarity. In this gun 5 indicates the cathode, 6 indicates the control grid, 7 the accelerating anode and 8 the anode. This portion of the gun produces an electron current which is already slightly beamedbut which is concentrated still further in order to obtain a very small focus. This concentration is effectedwith the use of

electrodes

9 and 10 which, together with the electrode 8, constitute a lens system. For this purpose it is, of course, necessary to apply suitable voltages to the electrodes 5 to 10 inclusive. However, this has no concern with the invention as such, since the gun is built up in a fully conventional way and also included in a circuit in known manner. It is thus also possible, for example, to utilize so-called triode systems, in which an accelerating anode is not present.

The cathode-ray tube shown comprises two sets of

deflection plates

11, 12 in the two outer electron guns. Furthermore, the figure shows a set of coils 13, 14 by which the three rays or beams produced by the electron guns are jointly deviated in one direction perpendicular to the plane of the drawing and caused to scan the screen so that the raster is written on the luminescent screen 4. The other set of coils for the deflection in the plane of drawing at right angles to said one direction is not shown for the sake of clarity. As will be noted, one deviation field component extends in the plane of the three guns but at right angles to their axes. By applying suitable direct voltages to the deflecting

systems

11, 12 it may be ensured that, in the rest or center positions, the three electron rays converge to meet at one point 15 at the centre of the luminescent screen 4. The device once thus adjusted, the three rays always meet substantially at one point, even if deviating currents are supplied to the deviation coils to cause the converged beams to scan the screen. In order to arrange for these points always to be located on the luminescent screen 4, it will in many cases be necessary for' the

deflection systems

11, 12 to be supplied, in addition, withcorrecting voltages, which are derived from the voltages providing the currents in the deviation. coils. tive, the luminescent screen 4 may be given a curvature such that the meeting point of the three rays is always located on. the luminescent screen without correcting voltages on the

deflection systems

11, 12. In this case it is necessaryonly to apply direct voltages to the deflecting systems 1 1, 12.

As pointed out before, thereis the possibility that the three electron rays or beams may not maintain their single planar relationship- Figs. 2 and 3 show a modification for restoring this relationship. The part of the device shown in these figures is that in the vicinity of the

deflection systems

11, 12. As illustrated,

magnets

22 and 23 can be provided alongside the envelope adjacent the two outer beams to provide magneticfields to correct the positions of the outer two beams, i. e.,

. adjust the positions of the outer two beams so. thatthey lie in a single flat plane with the center beam. To avoid influencing the course of the centernbeam, a ferromagnetic member 21 can be provided to surround the center beam and thus shield it from external magnetic fields. If desired, further shielding of the center beam can be obtained by constructing the electrode 10 also of ferromagnetic material.

What is claimed is:

1. An electrical device comprising a cathode-ray tube including an electron-receiving screen, means including three electron guns within said tubeproducing three electron beams lying in as single flat plane, deviation-fieldproducing means common to said three electron beams for causing said three beams in said single plane jointly to scan said, electron-receiving screen, said deviationfield-producing means establishing a field having substantially two perpendicular components, one of said perpendicular components being parallel to the single plane of the beams and also substantially at right angles to the axis of the tube, and electrostatic deflecting means associated with each of two of said electron guns for causing the beams produced by said two guns to be di rected substantially to the same area of said screen a the beam from the third gun. p

2. An electrical device as set forth in claim 1 wherein the three electron guns are located such that their axes intersect the screen at a common point.

3. An electrical device for producing color television images, comprising a cathode-ray tube including an electron-receiving screen, three electron guns within said tube and located substantially in a single flat planeand substantially parallel to one another, deviation-fieldproducing means common to, said, three electron beams for causing said three beams jointly, to scan said screen, said three electron beams lyingina single flat, plane when they traverse the deviation-field, said deviationfield-producing means producing a field within said tube constituted of two substantially perpendicular components, one of said components extending parallel to i However, as an alterna- 2,849,647 5 6 ing means includes a pair of flat deflection electrodes References Cited in the file of this patent associated with each of the two outer guns. UNITED STATES PATENTS i5. A device as set forth in claim 4 wherein magnets are provided to correct the position of the electron beams 2165028 'Blumlem July 1939 produced by the outer two guns, and means are provided 5 2170944 Gllass 1939 for shielding the electron beam produced by the central 2587'O74 sztklal 1952 gun from the fields producd by the magnets. 2679614 Fnend May 25, 1954 6. A device as set forth in claim 5 wherein at least 2761089 Haeff 1956 one electrode of the central electron gun is constituted of ferromagnetic material to shield the electron beam 10 produced thereby from the field produced by the magnets UNITED STATES PATENT OFFICE CERTIFICATE OF CORRECTION Patent No. 2,849,647 August 26, 1958 Jan Carel Erancken 1 It is hereby certified that error appears in the printed specification of the above numbered patent requiring correction and that the said Letters Patent should read as corrected below.

Column 3, line 34,- after the numeral 3" insert are column 4, line 38, for "as single" read a single 7' Signed and sealed this 25th cla; of November 1958.

( SEAL) Mtest:

KARL H.. A)CLINE ROBERT C. WATSON P ttesting Officer Y I I Commissioner of Patents UNITED STATES PATENT OFFICE CERTIFICATE OF CORRECTION 3atent No. 2,849, 64? August 26, 1958 Jan Care]. Francken It is hereby certified that error appears in the printed specification if the above numbered patent requiring correction and that the said Letters gatent should read as corrected below.

Column 3, line 34, after the numeral "3" insert are column 4, line 38, for "as single" read a single Signed and sealed this 25th day of November 1958.,

SEAL) ttest:

ARL H, AXI-INE ROBERT (J. WATSON tte'sting Officer 1 Commissioner of Patents