US2927233A - Electrical apparatus - Google Patents
Electrical apparatus Download PDFInfo
- Publication number
- US2927233A US2927233A US620517A US62051756A US2927233A US 2927233 A US2927233 A US 2927233A US 620517 A US620517 A US 620517A US 62051756 A US62051756 A US 62051756A US 2927233 A US2927233 A US 2927233A
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- US
- United States
- Prior art keywords
- insulating
- insulator
- electrode
- interelectrode
- anode
- 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 - Lifetime
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- 239000012212 insulator Substances 0.000 description 17
- 239000011324 bead Substances 0.000 description 7
- 230000015556 catabolic process Effects 0.000 description 7
- 238000000034 method Methods 0.000 description 6
- 230000005684 electric field Effects 0.000 description 3
- 239000011521 glass Substances 0.000 description 3
- 230000008021 deposition Effects 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 239000000126 substance Substances 0.000 description 2
- 230000001154 acute effect Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 238000011109 contamination Methods 0.000 description 1
- 230000006378 damage Effects 0.000 description 1
- 239000003989 dielectric material Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000010894 electron beam technology Methods 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 238000005755 formation reaction Methods 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 238000005286 illumination Methods 0.000 description 1
- 230000003116 impacting effect Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000155 melt Substances 0.000 description 1
- 239000010445 mica Substances 0.000 description 1
- 229910052618 mica group Inorganic materials 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 231100000572 poisoning Toxicity 0.000 description 1
- 230000000607 poisoning effect Effects 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
- H01J29/82—Mounting, supporting, spacing, or insulating electron-optical or ion-optical arrangements
Definitions
- This invention relates to evacuated electron discharge devices, and more particularly to improved interelectrode insulating arrangements employed therein.
- a factor which has considerable influence on the aforesaid brightness characteristics is the anode potential, this being largely determinative of the accelerating force impressed on the beam of electrons emitted from the cathode. Since the intensity of light emitted by phosphorescent materials is proportional to the excitation induced by the impacting electrons, and since the energy of the electron beam is directly proportional to the anode voltage, it is apparent that a contribution enabling the imposition of anode potentials higher than presently feasible would be most promising in solving the brightness problem. Moreover, increase of anode voltage has the additional advantage of advantageously affecting the spot size.
- any appreciable increase of the anode voltage over presently existing norms has resulted in high voltage breakdown, a condition which normally manifests itself in breakdown of the interelectrode insulating support means, as for example by fracturing of the interelectrode insulating bead or rod, or by high voltage arcing which takes place along the surface of one or more of the insulating support members.
- the invention is featured by the provision of an electron gun which is of very simple yet very rigid construction, and contemplates a unique design for overcoming certain of the limitations of prior art devices.
- Figure 1 is a plan view of an electron gun structure embodying the present invention, the structure being shown in position in the neck of a tube;
- Figure 2 is a side elevational view of the apparatus shown in Figure l;
- Figure 3 is a view'showing an alternate embodiment.
- the illustrated embodiment of the invention depicts an electron gun structure of the type used in cathode ray tubes, comprising a cathode, control grid and anode, the latter two elements being held in rigid axial alignment by insulating support members of high dielectric strength.
- the impasse in present design has been the absence of a method of preventing breakdown of the dielectric supporting members once high anode voltages have been imposed.
- Excellent insulators such as glass and mica, break down and carry current when a great enough voltage is applied, hence if a high enough electric field is impressed and maintained, the insulator becomes heated with the final result that some electrons leave their atoms. The electric field then urges the electrons through the substance of the insulator, resulting in a small leakage current.
- the partial breakdown of an insulator as described above, is rapidly followed by a complete breakdown; the current flowing through the insulator, even though small, generates more heat, thereby pyramiding its disruptive effect.
- a condition which further aggravates this problem of high voltage breakdown is the microscopic deposition of conductive materials on the surface of the insulating support structure. This deposition results from the gradual release of metal vapors and other substances occluded or absorbed within the various internal members of the tube assembly. This phenomenon produces a secondary electrical path along the surface of the insulating bead, and high voltage arcing which occurs via this route produces ionization of the residual gas particles within the tube, thereby deleteriously contributing to cathode poisoning, attrition of the emissive surface of the cathode and the condition known as ion spot. Moreover, original contamination of the insulator surface, even in the absence of the aforesaid conditions, provides a sufiiciently conductive path for high voltage arcing.
- an electron gun structure 9 disposed within a neck portion of a cathode ray tube, comprising the open oval shaped insulating beads or canes 10 and 11 whose function it is to insulate the control grid 12 from the extremely high voltages impressed on the anode 13, and to additionally maintain the necessary interelectrode spacing and desired rigid predetermined axial alignment of said electrode members.
- electrodeins'ulator junction is to be construed, for purposes of this invention, as. being the interface or point or" demarcation between the insulator and the conducting surface ofthe electrode element.
- the, electrode-insulator junctions are. the points at which the metal electrode tabs 16 join the insulators 1i and 11.
- an electrode assembly comprising, a plurality of electrodes, and elongated, generally rod-like, vitreous insulating means joined to and supporting said electrodes in spaced relation, the :length ,of said insulating means, between electrode-insulator junctions, being greater than the rectilinear distance between said junctions, and said insulating means being so shaped as to cause, in at least one portion thereof, distortion of its cross sectional configuration.
- an electrode assembly comprising, a plurality of generally tubelike electrodes, and elongated, vitreous insulating means joined to and supporting said electrodes in spaced, generally axial alignment, the length of said insulating means, between electrode-insulator junctions, being greater than therectilinear distance between said junctions, and said insulating means beingso shaped as to cause, in at least one portion thereof, distortion of its cross sectioni 7
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- Manufacture Of Electron Tubes, Discharge Lamp Vessels, Lead-In Wires, And The Like (AREA)
Description
March 1, 1960 e. F. BARNETT ETA]. 2,927,233
ELECTRICAL APPARATUS Filed NOV. 5, 1956 i F7c-I2.
INVENTORJ L My 5 EAR/V577 BY ao/wo/v A. rpm/rm United States Patent ELECTRICAL APPARATUS Guy F. Barnett, Ros! and Gordon R. Spencer, Lansdale, Pa., assignors to Philco Corporation, Philadelphia, Pa., a corporation of Pennsylvania Application November 5, 1956, Serial No. 620,517
3 Claims. (Cl. 313-64) This invention relates to evacuated electron discharge devices, and more particularly to improved interelectrode insulating arrangements employed therein.
Problems which have received considerable attention in the prior art, particularly in the case of television high illumination projection tubes, are those dealing with means for increasing the brightness of the phosphorescent screen and for improving the apparent contrast of objects imaged thereon. This problem is particularly acute in color television tubes where the efficiency of the phosphors is down nearly an order of magnitude from that found in black and white sets.
A factor which has considerable influence on the aforesaid brightness characteristics is the anode potential, this being largely determinative of the accelerating force impressed on the beam of electrons emitted from the cathode. Since the intensity of light emitted by phosphorescent materials is proportional to the excitation induced by the impacting electrons, and since the energy of the electron beam is directly proportional to the anode voltage, it is apparent that a contribution enabling the imposition of anode potentials higher than presently feasible would be most promising in solving the brightness problem. Moreover, increase of anode voltage has the additional advantage of advantageously affecting the spot size.
In attempting to accomplish either or both of the afore said objects, namely of increasing the brightness of a phosphorescent screen or reducing spot size, any appreciable increase of the anode voltage over presently existing norms has resulted in high voltage breakdown, a condition which normally manifests itself in breakdown of the interelectrode insulating support means, as for example by fracturing of the interelectrode insulating bead or rod, or by high voltage arcing which takes place along the surface of one or more of the insulating support members.
It has therefore become necessary, as a prerequisite to the use of higher operating potentials, to provide interelectrode insulating means that will withstand these desirable higher voltages.
It is consequently a primary object of this invention to provide a method of supporting the electrode elements within an electron gun structure of the type used in cathode ray tubes so as to prevent or mitigate high voltage breakdown of the interelectrode insulators.
In the illustrated embodiment, the invention is featured by the provision of an electron gun which is of very simple yet very rigid construction, and contemplates a unique design for overcoming certain of the limitations of prior art devices.
It is another object of this invention to provide a simple inexpensive means for overcoming prior art limitations, and for enabling the imposition of exceedingly high potential gradients between interelectrode elements of an evacuated electron discharge device.
These and other objects within contemplation will be 2,927,233 Patented Mar. 1, 1960 readily understood by reference to the following detailed description and the accompanying drawing in which:
Figure 1 is a plan view of an electron gun structure embodying the present invention, the structure being shown in position in the neck of a tube;
Figure 2 is a side elevational view of the apparatus shown in Figure l; and
Figure 3 is a view'showing an alternate embodiment.
First briefly described, the illustrated embodiment of the invention depicts an electron gun structure of the type used in cathode ray tubes, comprising a cathode, control grid and anode, the latter two elements being held in rigid axial alignment by insulating support members of high dielectric strength.
Given a fixed axial electrode spacing the impasse in present design has been the absence of a method of preventing breakdown of the dielectric supporting members once high anode voltages have been imposed. Excellent insulators, such as glass and mica, break down and carry current when a great enough voltage is applied, hence if a high enough electric field is impressed and maintained, the insulator becomes heated with the final result that some electrons leave their atoms. The electric field then urges the electrons through the substance of the insulator, resulting in a small leakage current. Generally the partial breakdown of an insulator, as described above, is rapidly followed by a complete breakdown; the current flowing through the insulator, even though small, generates more heat, thereby pyramiding its disruptive effect.
A condition which further aggravates this problem of high voltage breakdown is the microscopic deposition of conductive materials on the surface of the insulating support structure. This deposition results from the gradual release of metal vapors and other substances occluded or absorbed within the various internal members of the tube assembly. This phenomenon produces a secondary electrical path along the surface of the insulating bead, and high voltage arcing which occurs via this route produces ionization of the residual gas particles within the tube, thereby deleteriously contributing to cathode poisoning, attrition of the emissive surface of the cathode and the condition known as ion spot. Moreover, original contamination of the insulator surface, even in the absence of the aforesaid conditions, provides a sufiiciently conductive path for high voltage arcing.
When vitreous dielectric materials, such as glass, are employed as insulating support members, it has been found that in the manufacture of the insulating bead, numerous longitudinal capillary size passages are formed within the internal structure, caused by bubbles in the melt being elongated in the drawing operation. These capillaries contain gas under reduced pressure which ionizes when subjected to an electric field. This produces heating with attendant expansion of the entrapped gas, a condition ultimately leading to destruction of the vitreous insulator.
Regardless, however, of the reasons for insulator failure the fact remains that the unique structural design herein taught greatly extends the insulating range of such elements and enables the use of higher operating potentials within the evacuated electron discharge device.
Now making detailed reference to the drawing and particularly to Figure 2 thereof, there is shown an electron gun structure 9, disposed within a neck portion of a cathode ray tube, comprising the open oval shaped insulating beads or canes 10 and 11 whose function it is to insulate the control grid 12 from the extremely high voltages impressed on the anode 13, and to additionally maintain the necessary interelectrode spacing and desired rigid predetermined axial alignment of said electrode members.
said path without the necessity of. increasing the interelectrode spacing which would in turn necessitate lengthening'of the overall gun structure. The term electrodeins'ulator junction is to be construed, for purposes of this invention, as. being the interface or point or" demarcation between the insulator and the conducting surface ofthe electrode element. In the revised showing in Figure 1, for example, the, electrode-insulator junctions are. the points at which the metal electrode tabs 16 join the insulators 1i and 11.
This technique ofinterposing an insulator defining'an extended leakage path between members maintained at widely different potentials, without changing pro-existing physical parameters, has resulted in an insulating method characterized by simplicity of design and one which is readily adaptable to present structural embodiments. By using an insulating configuration, as depicted in the drawing, voltages of considerablygreater magnitude than presently attainable may be employed while still maintaining previous interelectrode spacing. The effective elongation of the leakage path between predee termined, fixed electrode-insulator junctions is the essence of the present invention, and when it is'realized that'the brightness factor of the phosphors is approximately proportional to the anode voltage, it will be apparent that the technique here shown, for enablingthe imposition of higher anode voltages than heretofore possible, has appreciable significance.
When employing glass, ceramics, or other vitreous materials, as the insulating media, it has often been 'found, as previously mentioned, that there is within. the irisulator rod an internal longitudinal gas filled capillary passage which serves to bridge the interelectrode gap. The electrode insulating method here shown obviates this problem, as well as those aforementioned, in that form-ation of the arcuate contours 17 and 18, as shown for instance in Figure 2, serve to distort the cross sectional configuration of positions 19 and 20 effectively collapsing these internal gas pockets, thereby preventing volt- 7 .We claim:
age-.breakdownii'esultin'g fromthis cause. It will, of course, be understood that any mode of deforming the bead structure in a plane substantially transverse to its longitudinal axis will beeifective in eliminating this particular cause of insulator failure, as for example by applying a torsional stress to the bead during the formative stage to thereby distort the bead cross section, collapsing any internalcapillarygas pocket. H p
. While a preferr'edembodiment of this invention has been shown and described, it will be understood that such'modifications and changes are contemplated as may come within the scope of the appended claims.
1. For an evacuated electron discharge device, an electrode assembly comprising, a plurality of electrodes, and elongated, generally rod-like, vitreous insulating means joined to and supporting said electrodes in spaced relation, the :length ,of said insulating means, between electrode-insulator junctions, being greater than the rectilinear distance between said junctions, and said insulating means being so shaped as to cause, in at least one portion thereof, distortion of its cross sectional configuration.
2. For an evacuated electron discharge device, an electrode assembly comprising, a plurality of generally tubelike electrodes, and elongated, vitreous insulating means joined to and supporting said electrodes in spaced, generally axial alignment, the length of said insulating means, between electrode-insulator junctions, being greater than therectilinear distance between said junctions, and said insulating means beingso shaped as to cause, in at least one portion thereof, distortion of its cross sectioni 7 References Cited the'file of this patent UNITED STATES PATENTS Epstein Jilly 14, 1942 Anderson Feb; 6, 1951 Anderson Sept. 11, 1951
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US620517A US2927233A (en) | 1956-11-05 | 1956-11-05 | Electrical apparatus |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US620517A US2927233A (en) | 1956-11-05 | 1956-11-05 | Electrical apparatus |
Publications (1)
Publication Number | Publication Date |
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US2927233A true US2927233A (en) | 1960-03-01 |
Family
ID=24486284
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US620517A Expired - Lifetime US2927233A (en) | 1956-11-05 | 1956-11-05 | Electrical apparatus |
Country Status (1)
Country | Link |
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US (1) | US2927233A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3085172A (en) * | 1959-03-11 | 1963-04-09 | Corning Glass Works | Cathode ray tube gun assembly |
US3619688A (en) * | 1969-03-28 | 1971-11-09 | Griffiths Electronics Inc | Electron gun with connector of alternate electrodes shielding intermediate electrode |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2289906A (en) * | 1939-10-31 | 1942-07-14 | Rca Corp | Cathode ray tube |
US2540835A (en) * | 1946-12-13 | 1951-02-06 | Bell Telephone Labor Inc | Cathode-ray device |
US2567359A (en) * | 1947-09-06 | 1951-09-11 | Bell Telephone Labor Inc | Electron discharge apparatus |
-
1956
- 1956-11-05 US US620517A patent/US2927233A/en not_active Expired - Lifetime
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2289906A (en) * | 1939-10-31 | 1942-07-14 | Rca Corp | Cathode ray tube |
US2540835A (en) * | 1946-12-13 | 1951-02-06 | Bell Telephone Labor Inc | Cathode-ray device |
US2567359A (en) * | 1947-09-06 | 1951-09-11 | Bell Telephone Labor Inc | Electron discharge apparatus |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3085172A (en) * | 1959-03-11 | 1963-04-09 | Corning Glass Works | Cathode ray tube gun assembly |
US3619688A (en) * | 1969-03-28 | 1971-11-09 | Griffiths Electronics Inc | Electron gun with connector of alternate electrodes shielding intermediate electrode |
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