EP0348571A1 - Cathode ray tube display monitor with stray magnetic field compensation - Google Patents
Cathode ray tube display monitor with stray magnetic field compensation Download PDFInfo
- Publication number
- EP0348571A1 EP0348571A1 EP88305986A EP88305986A EP0348571A1 EP 0348571 A1 EP0348571 A1 EP 0348571A1 EP 88305986 A EP88305986 A EP 88305986A EP 88305986 A EP88305986 A EP 88305986A EP 0348571 A1 EP0348571 A1 EP 0348571A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- coils
- ray tube
- cathode ray
- magnetic field
- crt
- 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.)
- Withdrawn
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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
- H01J29/003—Arrangements for eliminating unwanted electromagnetic effects, e.g. demagnetisation arrangements, shielding coils
-
- 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
- H01J29/72—Arrangements for deflecting ray or beam along one straight line or along two perpendicular straight lines
- H01J29/76—Deflecting by magnetic fields only
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J2229/00—Details of cathode ray tubes or electron beam tubes
- H01J2229/0007—Elimination of unwanted or stray electromagnetic effects
- H01J2229/0015—Preventing or cancelling fields leaving the enclosure
Definitions
- This Invention relates to a cathode ray tube monitor having means for reducing stray magnetic field produced in front of the screen.
- An object of the present invention is to provide a simple but effective solution which will mitigate the effect of the low frequency magnetic field in front of the CRT monitor without requiring more than two coils.
- a CRT monitor comprises a CRT display together with an electromagnetic yoke assembly for causing an electron beam or beams to scan across the screen of the CRT, and a pair of compensating coils mounted so as to oppose the stray magnetic field in front of the CRT screen caused by the electromagnetic yoke assembly, and is characterised in that the pair of compensating coils is located adjacent the electromagnetic yoke assembly with their axie non-parallel but substantially in the same plane, orientated so that the compensating magnetic field is increased on front of the CRT screen and reduced behind the CRT screen.
- the two coils are inclined with respect to one another so that their axes intersect at a point behind the CRT screen, preferably on the axis of the CRT and yoke assembly.
- CRT 1 is provided with an electromagnetic yoke assembly 2 for sweeping the electron beam over the surface of the phosphor layer on the inner surface of the screen 3.
- an electromagnetic yoke assembly 2 for sweeping the electron beam over the surface of the phosphor layer on the inner surface of the screen 3.
- a low frequency magnetic field S will often be found in front of screen 3, caused by stray fields from the yoke assembly 2.
- the stray field S approximates to that which would be produced by a magnetic dipole D positioned with its axis vertical and intersecting the axis 4 of the CRT.
- a cancellation coil placed in the position of dipole D and energised to produce an equal magnetic dipole of the opposite sense would give effective cancellation of the deflection yoke's stray field S.
- the glass bulb of the CRT prevents placement of a single cancelling coil.
- a pair of cancelling coils one above and one below the CRT bulb might be arranged to approximate to a vertically orientated dipole.
- the conical shape of the CRT bulb prevents placement of the cancelling coils with their axes coincident with one another and with the axis of the equivalent stray field dipole D. Complicated winding arrangements have been suggested to overcome this difficulty.
- the coils 5 and 6 are inclined so that their axes intersect on the axis 4 of the CRT.
- stray magnetic fields in the 1 KHZ to 400 KHZ frequency range at a distance 0.3m from the CRT screen can be reduced to less than 20mT/S dB/dt and less than 80 nT ⁇ B.
- the size of the coil, the number of turns, their angle of inclination, their positions and the amount of current will depend upon the particular CRT and can be found by simple experimentation but by inclining the coils in accordance with the present invention, optimum cancellation of the stray field can be obtained in a simple manner.
- the invention avoids the additional expense (and increased energy loss) involved if more than two compensation coils are used.
- the invention is suitable for colour and monochrome CRT display monitors.
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Video Image Reproduction Devices For Color Tv Systems (AREA)
Abstract
The stray low frequency magnetic field (S) from an electromagnetic yoke assembly (2) which is produced in front of the CRT (1) screen (3) is compensated with a pair of coils (5 and 6) whose axes are inclined to one another to intersect on the side of the coils remote from the CRT screen. Preferably the coil axes intersect on the axes of the CRT and are equally inclined thereto.
Description
- This Invention relates to a cathode ray tube monitor having means for reducing stray magnetic field produced in front of the screen.
- Although there is no scientific proof that stray magnetic fields at the front of a cathode ray tube (CRT) monitor are harmful to humans, there is a requirement in certain Countries that the stray fields in the 1 KHZ to 400KHZ frequency range (hereafter refered to a slow frequency magnetic fields) are reduced to below a particular value. Accordingly much effort has been expended by the CRT monitor industry over the last year or so to meet this requirement. The most common approach has been to use one or more coils to provide a compensating magnetic field which tends to cancel the undesired stray magnetic field. Examples of this approach are described in Finnish Patent Application 86148, PCT Applications WO87/05437 and WO87/060054, European Patent Applications 220777 and 235863, German Patent Application 3631023 and 3707829 and, US Patents 4634930, 4677344 and 4709220 and IBM Technical Disclosure Bulletin, June 1988 pp119 to 122. A second approach has been to use a magnetic shunt, as described in pending European application No 88105077.7 (IBM Docket KI9-87.005). Although the problem of a stray field has been analysed and is thought to be well understood, it is clear from the number of attempts to solve the problem that the solution is not as simple as it would appear. Furthermore, any solution should not add unduly to the cost of the CRT monitor.
- An object of the present invention is to provide a simple but effective solution which will mitigate the effect of the low frequency magnetic field in front of the CRT monitor without requiring more than two coils.
- As will be evident from the prior art, the use of one coil is not very effective and hence the suggestions for two or more coils. The problem is that generally more than two coils are believed to be necessary to obtain optimum compensation. We have discovered that by suitable positioning and orientating just two coils, effective compensation can be obtained.
- According to the invention, a CRT monitor comprises a CRT display together with an electromagnetic yoke assembly for causing an electron beam or beams to scan across the screen of the CRT, and a pair of compensating coils mounted so as to oppose the stray magnetic field in front of the CRT screen caused by the electromagnetic yoke assembly, and is characterised in that the pair of compensating coils is located adjacent the electromagnetic yoke assembly with their axie non-parallel but substantially in the same plane, orientated so that the compensating magnetic field is increased on front of the CRT screen and reduced behind the CRT screen. In other words, the two coils are inclined with respect to one another so that their axes intersect at a point behind the CRT screen, preferably on the axis of the CRT and yoke assembly.
- The invention will now be described, by way of example, with reference to the drawing, the single figure of which is a schematic illustrating the principle underlying the present invention.
- In the drawing, CRT 1 is provided with an electromagnetic yoke assembly 2 for sweeping the electron beam over the surface of the phosphor layer on the inner surface of the
screen 3. As is now well known, a low frequency magnetic field S will often be found in front ofscreen 3, caused by stray fields from the yoke assembly 2. - Effectively, the stray field S approximates to that which would be produced by a magnetic dipole D positioned with its axis vertical and intersecting the axis 4 of the CRT.
- In theory, a cancellation coil placed in the position of dipole D and energised to produce an equal magnetic dipole of the opposite sense would give effective cancellation of the deflection yoke's stray field S.
- In practice however, and as exemplified by the aforementioned prior art, the glass bulb of the CRT prevents placement of a single cancelling coil. As attempted in the prior art, a pair of cancelling coils one above and one below the CRT bulb might be arranged to approximate to a vertically orientated dipole. However, the conical shape of the CRT bulb prevents placement of the cancelling coils with their axes coincident with one another and with the axis of the equivalent stray field dipole D. Complicated winding arrangements have been suggested to overcome this difficulty.
- However, effective cancellation can be obtained by positioning the pair of coils 5 and 6 further from the screen than the ideal position and arranging the axes of the coils so that they are non-parallel but in the same plane : this increases the magnetic field towards the side of the
screens 3 and decreases it away from the screen. The cancelling magnetic field is represented by 7. - Preferably, the coils 5 and 6 are inclined so that their axes intersect on the axis 4 of the CRT.
- With the arrangement shown stray magnetic fields in the 1 KHZ to 400 KHZ frequency range at a distance 0.3m from the CRT screen can be reduced to less than 20mT/S dB/dt and less than 80 nT ΔB.
- Clearly the size of the coil, the number of turns, their angle of inclination, their positions and the amount of current will depend upon the particular CRT and can be found by simple experimentation but by inclining the coils in accordance with the present invention, optimum cancellation of the stray field can be obtained in a simple manner. The invention avoids the additional expense (and increased energy loss) involved if more than two compensation coils are used.
- The invention is suitable for colour and monochrome CRT display monitors.
Claims (3)
1. A cathode ray tube display monitor comprising a cathode ray tube display (1), an electromagnetic yoke assembly (2) for causing an electron beam or beams to scan across the screen (3) of the cathode ray tube, and a pair (5,6) of compensation coils for producing a magnetic field which tends to cancel a stray low frequency magnetic field (S) produced by the magnetic yoke assembly in front of the screen, characterised in that the coils (5,6) are positioned and inclined with respect to one another in such a way that their axes intersect on the side of the coils remote from the screen.
2. A monitor as claimed in claim 1, in which the axes of the pair of compensations coils intersect at the axis of the cathode ray tube.
3. A monitor as claimed in either preceding claims in which the axes of the coils are equally inclined to the axis of the cathode ray tube.
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP88305986A EP0348571A1 (en) | 1988-06-30 | 1988-06-30 | Cathode ray tube display monitor with stray magnetic field compensation |
JP8818889A JPH0246085A (en) | 1988-06-30 | 1989-04-10 | Cathode ray tube display device |
EP89303223A EP0349098A1 (en) | 1988-06-30 | 1989-04-18 | Cathode ray tube display monitor with stray magnetic field compensation |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP88305986A EP0348571A1 (en) | 1988-06-30 | 1988-06-30 | Cathode ray tube display monitor with stray magnetic field compensation |
Publications (1)
Publication Number | Publication Date |
---|---|
EP0348571A1 true EP0348571A1 (en) | 1990-01-03 |
Family
ID=8200124
Family Applications (2)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP88305986A Withdrawn EP0348571A1 (en) | 1988-06-30 | 1988-06-30 | Cathode ray tube display monitor with stray magnetic field compensation |
EP89303223A Withdrawn EP0349098A1 (en) | 1988-06-30 | 1989-04-18 | Cathode ray tube display monitor with stray magnetic field compensation |
Family Applications After (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP89303223A Withdrawn EP0349098A1 (en) | 1988-06-30 | 1989-04-18 | Cathode ray tube display monitor with stray magnetic field compensation |
Country Status (2)
Country | Link |
---|---|
EP (2) | EP0348571A1 (en) |
JP (1) | JPH0246085A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE4138526A1 (en) * | 1990-11-29 | 1992-06-11 | Murata Manufacturing Co | DEFLECTOR COIL FOR A TELEVISION |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2965769B2 (en) * | 1991-10-17 | 1999-10-18 | 三菱電機株式会社 | Cathode ray tube display device |
US5499004A (en) * | 1993-03-12 | 1996-03-12 | Matsushita Electric Industrial Co., Ltd. | Dielectric filter having interstage coupling using adjacent electrodes |
GB2293299A (en) * | 1994-09-15 | 1996-03-20 | Ibm | Electric field emission reduction system |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1987005437A1 (en) * | 1986-03-04 | 1987-09-11 | Autovision S. Blixt Ab | A device for the suppression of leakage fields in front of viewing screens and the like |
EP0258891A2 (en) * | 1986-09-05 | 1988-03-09 | Murata Manufacturing Co., Ltd. | Deflection yoke apparatus with means for reducing unwanted radiation |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE3017331A1 (en) * | 1980-05-06 | 1981-11-12 | Siemens AG, 1000 Berlin und 8000 München | ARRANGEMENT FOR COMPENSATING FOR MAGNETIC FOREIGN INTERFERENCE ON COLOR TV TELEVISIONS |
-
1988
- 1988-06-30 EP EP88305986A patent/EP0348571A1/en not_active Withdrawn
-
1989
- 1989-04-10 JP JP8818889A patent/JPH0246085A/en active Granted
- 1989-04-18 EP EP89303223A patent/EP0349098A1/en not_active Withdrawn
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1987005437A1 (en) * | 1986-03-04 | 1987-09-11 | Autovision S. Blixt Ab | A device for the suppression of leakage fields in front of viewing screens and the like |
EP0258891A2 (en) * | 1986-09-05 | 1988-03-09 | Murata Manufacturing Co., Ltd. | Deflection yoke apparatus with means for reducing unwanted radiation |
Non-Patent Citations (1)
Title |
---|
IBM TECHNICAL DISCLOSURE BULLETIN, vol. 30, no. 12, May 1988, pages 9-10, New York, US; "Cancellation of leaked magnetic flux" * |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE4138526A1 (en) * | 1990-11-29 | 1992-06-11 | Murata Manufacturing Co | DEFLECTOR COIL FOR A TELEVISION |
Also Published As
Publication number | Publication date |
---|---|
JPH048997B2 (en) | 1992-02-18 |
JPH0246085A (en) | 1990-02-15 |
EP0349098A1 (en) | 1990-01-03 |
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PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
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AK | Designated contracting states |
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17P | Request for examination filed |
Effective date: 19900419 |
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17Q | First examination report despatched |
Effective date: 19920403 |
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STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE APPLICATION HAS BEEN WITHDRAWN |
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18W | Application withdrawn |
Withdrawal date: 19920610 |