GB2208034A - Reducing magnetic radiation in front of a cathode ray tube screen - Google Patents

Description

1 1 1 MAGNETIC SHUNT FOR DEFLECTION YOKES

Field of the Invention

2f- C, ', 2 08 U 4 The present invention relates to display apparatus, and more particularly relates to apparatus for reducing unwanted magnetic radiation external to a cathode ray tube display device, in front of the screen thereof.

Background Art

Cathode Ray Tubes ("CRTs") generally have associated coils, or yokes, to provide a varying magnetic field for electron beam deflection, for example for raster scan. In addition to manifesting itself within the CRT, for beam deflection, this magnetic field also extends outside of the CRT, and even in front of the screen. This external magnetic field serves no useful purpose and an effort is frequently made to reduce this part of the yoke magnetic field.

Means to provide this reduction have been proposed in the prior art. For example, one such proposal is the provision of Helmholtz coils disposed "on top of", or radially away from and adjacent to the saddle-shaped deflection yoke. The coils are coupled to the deflection coils and the EMF is induced therein, giving rise to a magnetic field which tends to cancel the residual magnetic field in front of the screen. However, this is a relatively expensive and bulky solution to the problem.

Another proposed solution is the placement of shielding all around the CRT, which results in magnetic radiation reduction from the eddy currents induced in the shielding. However, this is also an expensive solution to the problem, and results in only minimal reduction in the magnetic field in front of the screen.

2 There is therefore a need for means to reduce to acceptable levels the residual magnetic field in front of the cathode ray tube display device that provides an inexpensive and compact solution to the problem.

Introduction to the Invention

Accordingly, the present invention provides a cathode ray tube apparatus comprising a viewing screen, means for producing a charged particle beam directed at the screen from the rear thereof, a deflection coil disposed behind the screen for deflecting the beam across the screen and means for reducing magnetic radiation in front of the viewing screen comprising magnetic shunt means disposed between the coil and the screen.

The present invention finds application in a cathode ray apparatus including a cathode ray tube ("CRV') having a screen for viewing and having a charged particle beam directed at the screen from the rear thereof and aligned with the central axis of the tube, but that may be magnetically deflected from the axis, and having a deflection coil producing a magnetic component from axially aligned wire segments and a magnetic component from circumferentially aligned wire segments relative to the axis, giving rise to a net distributed magnetic field in front of the coil. The apparatus reduces the net distributed magnetic radiation in front of the coil through the provision of a magnetic shunt disposed between the coil and the screen, wherein the magnetic shunt comprises a magnetically permeable material having its configuration and position relative to the coil selected to minimize the net distributed magnetic field in front of the coil.

The invention may be embodied in forms which are made of relatively inexpensive linear ferrite materials configured in shames that are inexpensive to provide, such as a flat ring or the like. As such, it permits a relatively inexpensive solution to the problem. in addition, 3 in tested embodiments the present invention has demonstrated dramatic reductions in the unwanted radiation in front of CRTs to which it has been applied.

Brief Description of the Drawings

Fig. 1 is a diagram showing pertinent portions of an integrated yoke tube component.

Fig. 2 is a simplified diagram of one winding each from the upper and lower deflection coils of the integrated yoke tube -component shown in Fig. 1.

Fig. 3 is a plot showing the magnetic field intensity along the Z axis for a typical deflection yoke such as is shown in Fig. 1.

Fig. 4 is a figure like that of Fig. 1, having added thereto a ring 50 in accordance with the preferred embodiment of the present invention.

Fig. 5 is a diagram like that of Fig. 2, having added thereto a ring 50 in accordance with the preferred embodiment of the present invention.

Fig. 6 is a plot showing the effective mu vs. actual mu for the ring depicted in Figs. 4 and 5.

Fig. 7 is a set of curves, on the same set of axes as in Fig. 3, showing the effect on the net field A of ring 50.

Fig. 8 is a set of curves showing the effect of ring 50 on the end turn field sho,sm in Fig. 3.

Fig.9 is an expanded view of the portion of the curve shc,,,..- in Fig. 7 beyond approximately 2.5 centimeters.

4 Fig. 10 is a plot like that of Fig. 9, wherein ring 50 is a slightly different distance from the yoke.

Fig. 11 is a diagram like Fig. 9, in which the inner diameter radius of ring 50 is slightly different from that of Fig. 9.

Fig. 12 is a curve like that of Fig. 9 but wherein the distance of the ring 50 from the end of the -yoke is different from that of Fig. 9 and Fig. 10.

Fig. 13 is a diagram of a further embodiment, which includes a lip portion 62.

Fig. 14 shows a still further embodiment in which a ring is provided having two portions.

Pig. 15 shows a still further embodiment made by injection moldina techniques of a material such as nylon impregnated with ferrite particles.

Fig. 16 is a cross-sectionai- diagram, through a portion of a still further embodiment of ring, made with conventional mu metal laminates.

Fig. 17 shows a further embodiment, having a hexagonal shape.

Detailed Description of the Invention

Fig. 1 shows the pertinent portions of an integrated yoke tube component ("ITC") 10 which includes a CRT 12, having a front screen 14, and upper and lower horizontal deflection coils 16, 18. The deflection coils 16, 18 generate a varying magnetic field between them, inside CRT 12, to deflect the electron bear. within the tube 12 for horizontal sweeping across the face of the screen 14, as is well known in the art.

i i 1 4 Fig. 2 is a simplified diagram of one winding each from the upper and lower deflection coils 16, 18, of Fig. 1. Thus, loop 20 is a single loop from coil 16, while loop 22 is a single loop from coil 18. As illustrated, a current i flows through each of the coils so as to generate the above described varying magnetic field for horizontal deflection of the electron beam. The useful portion of the loops 20, 22 are the axially aligned portions thereof 24, 26, 28, 30, which produce the main deflection field.

The circumferentially aligned portions of the loop (end turns) 32, 34, 36, 38 serve only to complete the circuit of each of the respective loops 20, 22, and are otherwise unnecessary for the operation of the deflection coils 16, 18. These circumferentially aligned coil portions 32, 34, 36, 38 contribute the major portion of the residual distributed magnetic field that extends a significant distance in front of the screen 14 (Fig. 1) which is to be reduced. In effect, the residual field is the vector sum of the main deflection field and the end turn field. The resulting sum will follow the polarity of the end turn field, since the end turn component is the larger, and both decav at the same rate with distance.

In Fig. 2, X, Y, and Z axes are depicted, having their origin in the plane of circumferential coil portions 34, 38 and centrally located between them. The Z axis coincides with the central axis of CRT 12 (Fig. 1). Note that the upper and lower halves 20, 22 are symmetrical about the x-z and y-z planes.

In actual operation the upper and lower loops 20, 22 are interconnected to produce a dipole field on the Z axis, as is known. From the known coil shape and current, the 9 field is given by:

9 p!-- dl 47r f 12x 6 where J is the current, R is the direction and R is the distance to a point of interest T on the Z axis.

A plot of the U field distribution of a typical horizontal deflection coil, such as is shown in Fig. 1, shielded with high permeability material, like ferrite, is shown in Fig. 3. The actual 9 field is a directional field, and the plot shown in Fig. 3 shows only the magnitude, or intensity, of such magnetic field along the Z axis. The units depicted on the horizontal axis are centimeters, while the units in the vertical axis are gauss. The curve reflects a typical coil having current flowing so as to produce a field which deflects a 20 kilovolt electron beam to an angle of about 40 degrees.

Curves A, B, and C of Fig. 3 represent the total field, the partial field from the axial wires and the partial field from the end turns, respectively. Curve A is the magnitude of the vector sum of the fields represented by curves B and C. In typical uncompensated vokes, at 55 centimeters in front of the yoke the field can be in range of approximately 1,000 - 2,000 nano-Tesla. Clearly, this is not a very large magnetic field. However, in accordance with the present invention this field can be reduced to an even smaller quantity. In actual experiments using the preferred embodiment described below, reductions to below 200 nano-tesla at 55 centimeters was measured.

Fig. 4 shows the ITC 10 of Fig. 1 having added thereto a ring 50 of linear ferrite operating as a magnetic shunt, in accordance with the preferred embodiment of the present invention.

Fig. 5 shows the loops 20, 22 of Fig. 2, with the ferrite ring 50 disposed in front of it, to illustrate the relative shape and position of ring 50.

7 Ring 50, as mentioned above, is a linear ferrite. Linear ferrite is a well known material commonly used in transformer and yoke production. According to the preferred embodiment the ring 50 has a relatively high magnetic permeability, or mu. It also has a high volume resistivity, or rho, for example 1 Meg ohm or more per cubic centimeter The high rho value keeps eddy currents at a minimum.

Otherwise the loading effects on the yoke would result in a need for more energy to drive the yoke. While embodiments could be constructed, for example out of conventional mu metal laminates, having this loading effect, and be in accordance with the present invention, it was deemed desirable to keep the eddy currents low, and avoid this loading effect in the preferred embodiment. The cross section of the ring 50 is large enough to avoid saturation.

Referring to Fig. 6 a plot is shown of the variation of effective mu, mu e versus actual mu, mu a? for a ring such as ring 50 positioned in front of coils 20, 22, as shown in Fig. 5. It can be seen that the effective mu rises abruptly for very low values of mu a and then reaches some point where it remains relatively constant in spite of ever increasing mu a- A value of 1,000 represents a point such as point 52 for a linear ferrite ring having dimensions typical for the application described herein. If a mu value of, for example, 10 were selected, it would be in the sloping area 53 of the curve shown in Fig. 6. Such a material would be highly susceptible to variations in manufacturing tolerances, temperature of operation, and the like, and would therefore provide erratic performance depending upon the variation of these factors. By selecting the permeability to be in the flat, horizontal area of the curve of Fig. 6, the above described undesirable variations in performance are substantially avoided. However, the material cost considerations will tend to keep the permeability of the material low within the range of acceptable permeability for providing this preferred stability.

1 8 Fig. 7 is a set of curves, on the same set of axes as these of Fig. 3, showing the effect on the net field A shown in Fig. 3 of a flat ring, such as ring 50 in Fig. 4, in accordance with the preferred embodiment of the present invention. Curve A in Fig. 7 is the same as curve A in Fig. 3. Curve D in Fig. 7 represents the field contribution from the magnetization effect of the ring 50, while curve E represents the resultant curve-from the combination of curves A and D.

To better understand the effect of the field from the ring on the overall magnetic field A, a set of curves is shown in Fig. 8 including curve D, the magnetic field from the ring, and two other curves which help in this understanding. Curve C is the same curve C as is shown in Fig. 3. Curve F is a curve representing the resultant field from. the combination of curves D and C. Note that in Fig. 8 the horizontal axis is the same as that of curves 3 and 7 while the vertical field has been expanded, to aid in clarity.

As mentioned above, curve D is the theoretical field of the ring alone. This is an intrinsic field which is created by the magnetisation force of the end turn field. It should be noted that the presence of the ring attenuates the end turn field. The degree of attenuation is controlled by the variables such as ring dimensions and ring yoke separation, as is discussed in more detail below. It should be further noted that the end turn field combines vith the main deflection field, and the area in front of the CRT screen, to form the net measurable residual field whose reduction is an object of this invention. At optimum attenuation, the modified end turn field F is equal in magnitude but opposite in direction to the main deflection fieldl resulting in a zero vector sum. As a practical matter, the net measurable residual field in front of the CRT screen can never be reduced to zero. However, by application of the principles of the present invention as disclosed herein, this field can be reduced to very small levels.

9 The portion of Fig. 7 beyond approximately 2.5 centimeters to the right thereof is shown in Fig. 9. In order to see clearly the curve behaviour in that region, the scale is expanded in the vertical direction as compared with Fig. 7. Curves A and E are as described in Fig. 7. Curve D is not shown in this figure in the interest of providing more clarity for curves A and E. Note that Curve E is very nearly at a zero field magnitude at approximately 9.5 centimeters.

The compensated curve E for a typical CRT-yoke configuration is shown, where the ring 50 is of ferrite with a permeability of 1,000 3,000, and a rho of 1 meg ohm per cubic centimeter or more, and having an inner dimension of 4 centimeters, a thickness of.2 centimeters, a width of 1 centimeter, placed at a distance of.4 centimeters from the end of the yoke. As used herein, the width of the ring refers to its radial extent from inner diameter to outer diameter.

Figs. 10-12 are plots like the plot shown in Fig. 9, for slightly different ring configurations from the configuration producing the curves of Fig. 9. Thus, in Fig. 10 all of the parameters for the ring are the same as those corresponaing to Fig. 9, except the distance of the ring from the end of the yoke. In Fig. 10 the curves correspond to a configuration in which this dimension is.3 centimeters. It will be appreciated that this reveals over-compensation, as the curve E' is slightly farther from the horizontal axis, for example at 9.5 centimeters.

The curves of Fig. 11 are for a configuration in which the dimensions are the same as those corresponding to Fig. 9, but wherein the inner diameter radius is 5 centimeters, instead of 4 centimeters. It can be seen that significantly less compensation is provided, as curve V' is here below the horizontal axis, and by an amount greater than curve E is above the horizontal axis, at 9.5 centimeters.

Fig. 12 shows a curve for a configuration wherein the dimensions are as in Fig. 9, but wherein the distance of the ring from the end of the yoke is.6 centimeters, instead of.4 centimeters. It can be seen that slightly less compensation is provided, causing curve Ell' to cross the horizontal axis at 9.5 centimeters. This was deemed to represent optimum compensation.

while curves are not provided showing the effect of change of width of the ring on the compensation effect, in general, decreasing the width will tend to reduce the compensating effect, while increasing the width will tend to increase the effect.

Thus, from the above Pigs. 9-12, it will be appreciated that changing the various dimensional parameters of the preferred embodiment of the present invention affects the performance of the ring in compensating by cancelling the magnetic field components on the Z axis in front of the screen due to yoke winding components. Through an understanding of these effects, one practicing the present invention can provide the adjustments deemed desirable to optimize the cancellation effect.

In an actual prototype experiment, in conjunction with an iTC manufactured by Matsushita Company having a series number of M34JDJ00X01, a ferrite ring of ordinary linear ferrite was provided, having a mu of approximately 1,000 - 3,000 and a rho of greater than 1 meg ohm per cc, ring dimensions of: an inner dimension of 4-3/8", a width of 3/8", and a thickness of 1/8". This ring was found to produce excellent cancellation effects when it was placed against the circumferential wire portions of the yoke provided with this ITC with spacing resulting only from the insulation of the yoke wires.

It should be noted that other configurations in accordance with the present invention may be used. For example, as shown in Fig. 13, a ring having a lip portion 62, may be employed to advantage, the lip 62 1 11 11 being believed to serve to enhance the cancellation of the undesired field. However, the additional machining required to make the configuration shown in Fig. 13 results in a more costly article than ring 50.

Another alternative configuration is that of a ring formed from two portions, such as is shown in Fig. 14.

Further, using injection molding techniques, for example with nylon impregnated with ferrite particles, a ring configuration having a cross section, such as is shown in Fig. 15 is also possible. It is believed that this configuration also provides beneficial cancellation field shaping characteristics. However, it also represents a more costly article than a simple flat ferrite ring such as described above.

Fig. 17 shows a hexagonally shaped ring, representing a still further embodiment for use withl for example, a hexagonally configured yoke.

Finally, embodiments may be made with conventional mu metal laminates, yielding rings having a cross-section as shown in FiQ. 16.

12

Claims (9)

1. A cathode ray tube apparatus comprising a viewing screen (14), means for producing a charged particle beam directed at the screen from the rear thereof, a deflection coil(16,18) disposed behind the screen for deflecting the beam across the screen and means for reducing magnetic radiation in front of the viewing screen comprising magnetic shunt means (50) disposed between the coil and the screen.

2. An apparatus as in claim 1 in which the magnetic shunt means comprises a ring of magnetically permeable material positioned adjacent the coil.

3. An apparatus as in claim 2 in which the deflection coil is a saddle coil and the ring is flat, formed of linear ferrite and abutting end turns of the saddle coil.

4. An apparatus as in claim 2 or claim 3 in which the ring has a rectangular cross-section.

5. An apparatus as in claim 2 or claim 3 in which the ring has an Lshaped cross-section.

6. An apparatus as in claim 2 or claim 3 in which the ring is of rounded cross-section, concave in the direction of the coil.

7. An apparatus as in any of claims 2 to 6 in which the ring comprises multiple section.

j 13

8. An apparatus as in any preceding claim in which the magnetic shunt means is formed of linear ferrite having a permeability such that the effective mu for its configuration and position varies little with variations in its actual mu.

9. An apparatus substantially as hereinbefore described with reference to the associated drawings.

Published 1988 at The Patent Office. State House. 66 71 High Rolborn, London WC1R 4TP. Further copies may be obtained from The Patent Office, Sales Branch. St Mary Cray, Orpington. Kent BR5 3RD. Printed by Multiplex techniques ltd, St Mary Cray, Kent. Con. 1.87