Background of the Invention
1. Field of the Invention
The present invention generally relates to a means for inhibiting radio frequency (RF) emissions from a cathode ray tube (CRT) display face and, more particularly, to an RF emission inhibiting means located at the rear surface of the CRT envelope.
2. Description of the Prior Art
The large aperture usually required by a CRT display in the wall of an otherwise well-shielded enclosure presents a potential shielding deficiency. Internally generated electromagnetic energy may be transmitted through such an aperture with relatively minor attenuation. RF emissions have generally been combatted by using a transparent conducting screen to cover the face of the CRT. The conductive screen may comprise either a wire mesh or a thin homogenous layer. The screen is bonded along its entire periphery to the enclosure wall, thus completing a conducting envelope surrounding all potential radiators.
Unfortunately wire meshes and homogeneous layers have practical limitations when the restrictions on RF emission are severe. Brightness and spatial resolution penalties result with the use of a wire mesh. Moreover, annoying moire patterns are formed as a consequence of the interaction of the geometric periodicity of the mesh and the raster scan lines or dot matrix CRT phosphor geometry. A homogenous conductive film generally comprises either metallic gold or indium-tin-oxide (ITO). The homogenous conductive film must be made thicker to increase shielding effectiveness. Optical transparency of the homogenous conductive film diminishes with increased thickness and therefore a compromise on thickness is usually made which is neither satisfactory in terms of transparency nor satisfactory in terms of RF emission shielding.
The inherent problems with a transparent conducting screen for shielding RF emissions from a CRT display face can be anticipated to have an ever increasing impact on the electrical and optical performance of display systems of evolving bandwidth, optical resolution, and physical size. Transparent conducting screens have a high material cost and require a high labor cost because of the delicate bonding operations.
U.S. Pat. No. 2,217,409 to Hepp is directed to a CRT control apparatus and discloses sheathing the deflection coils with conductive material comprising wound wire. An electrostatic screen made of helically wound non-magnetic material separates the inner pair of deflection coils from the outer pair. The whole of the coil system is surrounded by a helically wound sheath of magnetic material which closes the lines of force and is coaxial with the neck of the CRT. U.S. Pat. No. 3,824,515 to Holman shows a cylindrical electric screening used in the deflection units of CRTs. The electric cage comprises two adjacent helically wound wires with one end of each wire being connected to ground and the grounded ends being located at opposite ends of the neck tube of the CRT.
U.S. Pat. No. 2,567,874 to Cage and U.S. Pat. No. 2,623,923 to Zimmerman employ Faraday cages comprising longitudinal conductors disposed in an essentially cylindrical geometry. The longitudinal conductors are shown on the inside of a CRT envelope in the Cage patent. The purpose of Cage's arrangement is to provide a better electron return path within the CRT so that higher accelerating potentials can be applied resulting in increased brightness. The arrangement also shields the electron beam from exterior electric fields. The patent to Zimmerman is directed to an electrostatically shielded magnetic well logging system. The Faraday cage permits electromagnetic coupling between a sensitive measuring system and earth formations adjacent a well bore and prevents electrostatic coupling.
U.S. Pat. No. 4,392,083 to Costello shows a radiation shield for a CRT neck which shields proximate conductors from neck emissions. a plurality of elongated, coaxially oriented, spaced, conductive elements are bonded to the inner surface and outer surface of a sleeve of insulating material. The inner conductive elements are offset from the outer conductive elements. A conductive ring is connected to each of the inner elements and outer elements at one end of the sleeve and the ring is connected to ground potential by a drain strap. The neck shield disclosed in the Costello patent renders electromagnetic radiation from the CRT neck greatly attenuated while the magnetic field generated by the yoke is allowed to pass through the shield with relatively low attenuation.
There is no teaching in the prior art of a means for shielding RF emissions from the display face of a CRT which entirely avoids the need for an optically transparent screen in front of the display face of the CRT. Moreover, there is no teaching which anticipates moving the RF radiation barrier from its conventional location in front of the CRT face to the rear surface of the CRT envelope.
Summary of the Invention
It is therefore an object of this invention to provide an alternative method of shielding RF emissions from CRT displays which eliminates the need for an optically transparent screen in front of the face of a CRT display.
It is a further object of this invention to provide an RF emission shield of inverted topology wherein a shield at the rear of the CRT envelope prevents RF emissions from the face of the CRT display.
It is a further object of the invention to provide a RF emission shield of lower material and labor cost.
According to the invention, the CRT neck is surrounded by a conducting surface which acts as a cylindrical waveguide. The waveguide is coaxially aligned with the neck of the CRT and contiguous with it in order to act as a high pass filter. Electromagnetic energy with a frequency below the waveguide cutoff, which includes frequencies less than one gigahertz (GHz), is suppressed. In this invention, transmission of energy at frequencies associated with the video waveform including lower order harmonics are highly attenuated by the waveguide, thus frustrating egress of radiation from the CRT display face at these frequencies.
The potential sources of undesired RF emission are included in the video circuitry itself. For example, video amplifiers and video drivers emit electromagnetic energy which can be transmitted with relatively slight attenuation through an unshielded CRT display face. Generally the modulated electron beam current in the CRT does not play a significant role in the emission of RF energy by virtue of its minute absolute value. Usually no correlation is found between the video associated RF energy observed external to unshielded or poorly shielded displays and the brightness setting which is related to the average beam current. Even in a dark display with the electron beam biased completely OFF there is ordinarily no perceptible diminution of video related RF energy.
Problems are associated with placing a waveguide on the CRT neck. The interposition of a continuous isotropically conducting waveguide wall between the deflecting coils and the electron beam would effectively shield the electron beam from the deflection field itself. Additionally, the waveguide would behave as a shorted-turn secondary winding on a transformer whose primary winding is the deflection coil. Therefore, the shield has been constructed to avoid the associated problems while permitting the high pass action characteristic of the waveguide for various potential waveguide modes.
The shield comprises a set of narrow, parallel, longitudinal conductors which hereinafter will be called fingers and a set of narrow, parallel, circular conductors which hereinafter will be called hoops. The fingers bestow only the longitudinal conductivity required to support the transverse magnetic (TM.sub.01, TM.sub.02 . . . ) guide modes. The hoops yield the circumferential conductivity needed to support the transverse electric (TE.sub.01, TE.sub.02 . . . ) guide modes. The sets of fingers and hoops are not joined together electrically except along a single longitudinal finger if necessary for mechanical support or for facilitating fabrication. The longitudinal fingers can be connected together electrically at one end but not both ends. This topology prevents the formation of paths in which eddy currents could be induced by the deflecting fields but, at the same time, it would endow the shield with both longitudinal and circumferential conductivities. For transverse magnetic (TM.sub.01, TM.sub.02 . . . ) mode suppression, the longitudinal conductivity provided by the fingers is sufficient. For transverse electric (TE.sub.01, TE.sub.02 . . . ) mode suppression, however, only the circumferential conductivity due to the hoops is effective.
Although the Costello patent noted in the prior art is explicitly concerned with the shielding of proximate conductors from neck emissions and consequent re-radiation from the latter, the structure as described would also thwart the egrees of transverse magnetic (TM.sub.01, TM.sub.02 . . . ) mode radiation through the display face of the CRT. The geometry proposed by Costello would form a circular waveguide operated below cutoff and would therefore effectively attenuate a forwardly propagating wave, but the Costello patent makes no reference to the role of this mechanism. Moreover, the geometry in Costello would not suppress transverse electric (TE.sub.01, TE.sub.02 . . . ) mode radiation. Asymmetries, principally caused by off-axis conductors associated with the electrodes and adjacent circuits, can cause transverse electric mode excitation. The hoops are critical in the case of CRTs having asymmetrical arrangements of leads which extend inside the neck of the CRT.
RF emissions from a CRT housing are suppressed by a shielded enclosure which contains the CRT envelope wherein the CRT envelope has a waveguide neck shield and a non-shielded CRT face. Alternatively, the sources of potential undesired emission are contained within their own enclosure near the CRT base and this enclosure is bonded to the neck shield on the CRT. The alternative shielding configuration would eliminate the requirement for shielding the entire CRT housing.
Brief Description of the Drawings
The foregoing and other objects, aspects and advantages of the invention will be better understood from the following detailed description of the preferred embodiments of the invention with reference to the accompanying drawings, in which:
FIG. 1 is a three dimensional view of the sets of fingers and sets of hoops which comprise the RF emission shield according to the invention;
FIG. 2 is a plan view of a shielded CRT enclosure which may be used in combination with the invention; and
FIG. 3 is a plan view of an alternative shielded video circuit enclosure which may be used with the invention.
Detailed Description of the Preferred Embodiments of the Invention
Referring now to the drawings, and more particularly to FIG. 1, the RF emission shield according to the invention is shown generally at 8 as comprising a set of fingers 10 and a set of hoops 12. The finger set 10 comprises a plurality of narrow, parallel, longitudinally conductive fingers. Orthogonal to the finger set 10 is the hoop set 12 which comprises a plurality of narrow, parallel, circumferentially conductive hoops. The finger set 10 provides the longitudinal conductivity required to support the transverse magnetic guide modes. Below the cutoff frequency the finger set 10 suppresses only transverse magnetic mode radiation. The hoop set 12 yields the circumferential conductivity required to support the transverse electric guide modes. Below the cutoff frequency the hoop set 12 suppresses only transverse electric mode radiation. The finger set 10 and the hoop set 12 are not joined together electrically except at allowed electrical junctions 14 which give mechanical support and facilitate the RF emission shield's fabrication. The allowed electrical junctions 14 occur between a single longitudinal finger 16 and the all the hoops of the hoop set 12 and also, all the fingers of the finger set 10 are connected at one end 18 of the hoop set 12 but not both ends. The finger set 10 and the hoop set 12 may be printed on opposite sides of a flexible dielectric support using well known and conventional printed circuit techniques.
The shield thus described may be employed in a typical CRT display. The following dimensions are given to indicate a practical geometry:
Conducting material thickness: 0.003 inches
Finger or Hoop width: 0.038 inches
Center to Center Finger/Hoop Spacing: 0.058 inches
Insulation thickness: 0.002 inches
Length of Finger System: 2.00 inches
Diameter of Finger Stock: 1.18 inches
TM.sub.01 Mode Cutoff Wave Length: 2.61 a
TE.sub.01 Mode Cutoff Wave Length: 1.64 a
where a is the Guide Radius
In the example given, the corresponding cutoff frequencies will be; TM.sub.01 equal to 7.7 GHz and TE.sub.01 equal to 12.2 GHz. Below these frequencies mode propagation will be attenuated.
As best shown in FIG. 2, the RF emissions from a CRT display housing 20 are thwarted by a shielded enclosure 22 and the RF emission shield 8. The RF emission shield 8 is located coaxially with the neck of the CRT 24. The RF emission shield 8 is interposed between the neck of the CRT 24 and the deflection coils 25. The RF emission shield 8 prevents the egress of electromagnetic radiation from the non-shielded CRT face 26 and does not shield the electron beam from the deflection field itself. The RF emission shield 8 negates the need for a transparent conductive screen, not shown, to be placed in front of the CRT face 26. A transparent conductive screen would need to be bonded to the shielded enclosure 22 to prevent the egress of electromagnetic radiation from the CRT 24.
An alternative embodiment for thwarting RF emissions from a CRT display housing 20 is best shown in FIG. 3. An internal enclosure 28 shields RF emissions from the various sources of potential undesired emissions found in the video circuitry. The internal enclosure 28 is bonded to the RF emission shield 8. The alternative configuration eliminates the requirement for shielding the entire enclosure.
While the invention has been described in terms of the preferred embodiment which combines a set of longitudinally conductive fingers with a set of circumferentially conductive hoops to eliminate both transverse magnetic (TM.sub.01, TM.sub.02 . . . ) mode and transverse electric (TE.sub.01, TE.sub.02 . . . ) mode radiations from the CRT display face, those skilled in the art will recognize that the configuration of the fingers and hoops may be varied in the practice of the invention within the spirit and scope of the appended claims.