This invention generally relates to a cathode-ray tube (CRT) and, more particularly, to a tension mask having transverse scan.
A color picture tube includes an electron gun for generating and directing three electron beams toward a screen of the tube. An external magnetic deflection yoke subjects the three electron beams to magnetic fields that cause the electron beams to scan horizontally and vertically in a rectangular raster over the screen. The screen is located on the inner surface of the faceplate of the tube and comprises an array of elements of three different color emitting phosphors.
An aperture mask is interposed between the electron gun and the screen to permit each electron beam to strike only the phosphor elements associated with that beam. The aperture mask is a thin sheet of metal, such as steel or a nickel-iron alloy (INVAR®), that is parallel with the inner surface of the tube faceplate. The aperture mask may be either formed or tensioned.
Some cathode-ray tubes (CRTs) include high aspect ratios for the viewing screen (e.g., an 16:9 aspect ratio). Such high aspect ratios for the viewing screen requires the magnetic deflection yoke to use high deflection angles for scanning horizontally and vertically in a rectangular raster across the screen of the tube. High deflection angles for scanning horizontally and vertically in a rectangular raster across the screen increases the current requirements for the deflection yoke. A high current requirement for the deflection yoke undesirably increases the complexity and cost of such deflection yoke and chassis electronics as well as the power consumption required to operate the cathode ray tube.
Thus, a need exists for a cathode-ray tube including a high aspect ratio for the viewing screen with improved current requirements for the magnetic deflection yoke.
The present invention relates to a high aspect ratio cathode-ray tube (CRT) including a luminescent screen, an aperture mask configured for transverse scan, an electron gun and a magnetic deflection yoke. The electron gun and the magnetic deflection yoke are positioned so that electron beams generated in the gun scan a rectangular raster across the luminescent screen parallel to the tube minor axis (transverse scan) to improve the current requirements for the magnetic deflection yoke.
The aperture mask configured for transverse scan is interposed between the electron gun and the screen to permit each electron beam to strike only phosphor elements associated with that beam. The aperture mask is a tensioned mask having a center portion and edge portions. The center portion has a central frequency distribution and the edge portions have peripheral frequency distributions. The central frequency distribution is greater than the peripheral frequency distributions. The frequency distribution from the edge portions to the center portion is represented by a parabolic formula in which the variational range, Δ, between the peak value for the frequency distribution at the center portion and the minimum value for the frequency distribution at the edge portions is in the closed interval of about 8 Hz ≦Δ≦12 Hz.
The teachings of the present invention can be readily understood by considering the following detailed description in conjunction with the accompanying drawings, in which:
To facilitate understanding, identical reference numerals have been used, where possible, to designate identical elements that are common to the figures.
The tube 10 is designed to be used with an external magnetic deflection yoke, such as the yoke 34 shown in the neighborhood of the funnel-to-neck junction. When activated, the yoke 34 subjects the three beams to magnetic fields which cause the beams to scan vertically and horizontally in a rectangular raster across the screen 28 with transverse scan to improve the current requirements of the cathode-ray tube (CRT) 10.
The tension mask-frame assembly 30 configured for transverse scan, shown in greater detail in
Specifically, the aperture portion of tension mask-frame assembly 30 illustrated in
The natural frequency distribution across any complete vertical (central minor axis, Y) dimension of the tension mask 30 provides a useful way of comparing any tube to any other tube, regardless of size. Effectively, the natural frequency distribution, which is a function of the respective tension distribution and the horizontal dimension of the tension mask 30, is a universal metric that dictates the microphonic behavior of tubes.
The natural frequency distribution for transverse scan across the central minor axis, Y, is a substantially parabolic function that is substantially smooth and continuous. The natural frequency distribution comprises a central frequency distribution for the center portion 50 and peripheral frequency distributions for the edge portions 51, wherein the values of the central frequency distribution are constructively greater than the values of the peripheral frequency distribution. The difference between the maximum of the central frequency distribution and the minimum of the peripheral frequency distribution is preferably about 10 Hz.
When the center portion 50 is under greater tension than the mask edge portion 51, the condition is called a mask “frown”. A mask “frown” has a fundamental mode of vibration that principally involves the edge portion 51 of the mask 30. Border damping systems (BDS), i.e., vibration dampers, can effectively damp vibrational energy because the BDS are triggered by vibrations in the edge portion 51 of the mask 30.
When the center portion 50 is under less tension than the mask edge portion 51, the condition is called a mask “smile”. As such, the values of the central frequency distribution are less than the values of the peripheral frequency distribution. For a “smile” condition the damping of vibrations tend to be poor because the vibrating mask 30 has a fundamental mode dominated by the motion of the center portion 50 and does not trigger the BDS.
When the natural frequency distribution is even or flat, the values of the central frequency distribution and the peripheral frequency distribution are substantially similar. This example is difficult to implement. In addition, a slight change in tension distribution caused during manufacture of the tension mask 30 or during cathode ray tube operation could produce a “smile”, which is undesirable.
A tension mask 30 having a “frown” has resonant frequencies that are more broadly spaced than a tension mask 30 having a “smile” or flat distribution. Thus, when there is a vibration, energy from the first mode of the disturbance does not feed the second mode, thereby not prolonging the vibrational effect.
A tension distribution configured for transverse scan in accordance with the present invention for producing a parabolic “frown” at frequencies within a range of about 80 Hz to about 90 Hz, may be represented by:
where f(y) represents the frequency distribution over y (minor axis, Y), L represents one-half of the total length of tension mask 30 along the minor axis, and y represents a minor axis position from −L to +L, wherein the absolute value of L is normalized to 1. The preferred embodiment has the following provisions:
92≧A≧88 Expression 2
12≧B≧8 Expression 3
12≧f(ymax)−f(ymin)≧8 Expression 4
f(ymax) and f(ymin) represent the peak value of the frequency distribution at the center portion 50 and the minimum value of the frequency distribution at the edge portion 52, respectively. It is preferred that at least an 8 Hz differential be maintained between the frequency distribution at the center portion 50 and the edge portion 52.
When the mask frequency vibrations occur at or near a scan frequency or at or near a harmonic, a beating effect would result, wherein low amplitude modulation becomes perceptible.
Furthermore, because vibration amplitude is inversely proportional to mask tension, it is desirable to have overall mask tension as high as possible. The 10 Hz edge-to-center differential prescribed in Expression 4 provides a desirable solution to minimizing vibration while preserving the necessary “frown” tension distribution.
Additionally, there is a hierarchical relationship among the various tube sizes, wherein tubes using transverse scan require higher mask stress loads to achieve the desired frequency distribution than tubes using horizontal scan. For example, a W76 30-inch cinema screen tube using transverse scan experiences higher mask stress and frame load than a W76 30-inch cinema screen tube using horizontal scan at frequencies of about 80 Hz to about 90 Hz. The W86 34-inch cinema screen tube using transverse scan experiences higher mask stress and frame load than a W86 34-inch cinema screen tube using horizontal scan at frequencies of about 80 Hz to about 90 Hz. Similarly, the W97 38-inch cinema screen tube using transverse scan experiences higher mask stress and frame load than a W97 38-inch cinema screen tube using horizontal scan at frequencies of about 80 Hz to about 90 Hz.
As the embodiments that incorporate the teachings of the present invention have been shown and described in detail, those skilled in the art can readily devise many other varied embodiments that still incorporate these teachings without departing from the spirit of the invention.
This application is a continuation-in-part of co-pending U.S. patent application Ser. No. 09/797,229, entitled “A TENSION MASK FOR A CATHODE-RAY TUBE WITH IMPROVED VIBRATION DAMPING”, filed on Mar. 1, 2001, which is herein incorporated by reference.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/US03/26029 | 8/20/2003 | WO | 2/8/2006 |