[0001] This invention relates to color cathode ray tubes having aperture masks, and more
particularly relates to improved internal magnetic shields for such tubes.
[0002] Color cathode ray tubes for color television (color picture tubes) employing aperture
masks are known to be sensitive to external magnetic fields, especially the earth's
magnetic field, which can undesirably influence the trajectories of the electron beams,
causing shifting and distortion of the screen raster, as well as degradation of colour
purity and convergence. For example, shifting of a beam trajectory to the right or
left will result in a beam landing error in a tube with vertically oriented phosphor
stripes. That is, the beam will land to the right or left of the intended landing
area on the stripe.
[0003] For acceptable performance, therefore, such tubes must have effective shielding from
these magnetic fields, and it has become conventional practice to incorporate internal
magnetic shields into color picture tubes for this purpose.
[0004] Because the effect of theearth's magnetic field depends upon thelocation and orientation
of the tube, optimum shielding requires the ability to remagnetize the shield to realign
the magnetic domains after the tube has been moved. Accordingly, these shields are
customarily fabricated from a soft magnetic material, such as low carbon steel, enabling
ready remagnetization each time the television set is turned on.
[0005] The shape of the shield is in general dictated by the desire to have as much of the
tube volume shielded as possible, without having the shield interfere with the tube's
operation. For example, extending the shield too far back into the funnel risks interference
with the magnetic deflection field for the electron beams, as well as physical interception
or "clipping" of the deflected beams. In addition, cost considerations dictate as
simple a shape as possible.
[0006] In U.S. Patent 3,867,668, the shield is composed of two curved sheets of magnetic
material, said to make processing, storing, transportation and assembly convenient
and easy. In addition an external shield is employed to cover the gaps created by
the opening between the two curved sheets "to provide complete shielding".
[0007] It is customary to describe the effect of the earth's magnetic field on beam landing
interms of two components; the east-west effect, determined by a transverse horizontal
field, and the north-south effect, determined by an axial horizontal field. The magnitude
of these effects is the difference between the beam landing errors in the east and
west-facing directions, and the north and south-facing directions, respectively. It
is also customary to describe the tube's surface in terms of the face of an analog
clock. Thus, the top is 12 o'clock, the bottom is 6 o'clock, the right side (as seen
by the viewer) is 3 o'clock and the left side is 9 o'clock.
[0008] It is an object of the invention to provide improved internal magnetic shields for
color tubes which exhibit improved shielding and which can be readily fabricated using
present manufacturing techniques.
[0009] In accordance with the invention, an improved internal magnetic shield is provided
for a color tube comprising a bowl-shaped structure having at least one slot-shaped
opening in both the 6 and 12 o'clock sides of the shield, each slot aligned in the
direction of the axis of rotation or Z axis of the tube, and a large aperture surrounding
the Z axis for passing the tube's electron beams.
[0010] In accordance with a preferred embodiment, there is a pair of slots centrally located
and facing each other above and below the Z axis in the 6 and 12 o clock sides of
the shield.
[0011] In accordance with another aspect of the invention, such an improved shield is fabricated
by first cutting slots into a foil sheet of soft magnetic material, such as low carbon
steel, and then forcing the sheet over a bowl-shaped form to simultaneously stretch
and crimp the sheet into a bowl-shaped structure. Subsequently, an aperture is cut
into the shield.
Fig. 1 is a sectioned elevation view of a color picture tube incorporating an improved
internal magnetic shield according to the invention;
Fig. 2 is a plan view of the shield of Fig. 1 as seen from the rear, showing the slots
and the shield aperture; and
Fig. 3 is a side view of the shield of Fig. 1, showing the edge contour of one end
region of the shield aperture.
[0012] Referring now to Fig. 1, there is shown a color cathode ray tube for color television
(color picture tube) 11, including glass envelope 13 comprising an integration of
face panel 15, funnel 17 and neck 19 regions. Disposed on the interior surface of
face panel 15 is cathodoluminescent screen 21, consisting of an array of discrete
phosphor elements. Positioned in the neck 19 is mount 22 including an electron gun
for generating and directing three electron beams to screen 21. Positioned adjacent
screen 21 is a multi-apertured mask 25 for directing the electron beams to the desired
phosphor elements on the screen. Aperture mask 25 is supported by frame member 29,
which is in turn supported by studs 27 embedded in the sidewall of panel 15. Attached
to mask frame 29 is internal magnetic shield (IMS) 31 comprised of bowl-shaped structure
39 defining superjacent slots 41 in the centers of facing top and bottom sidewalls
thereof, aligned with the rotational or Z axis of the tube, and also defining aperture
47 surrounding the Z axis.
[0013] As can be seen from Fig. 1, the bowl-shaped structure 39 of shield 31 extends from
the periphery of the mask 25 downward along the funnel 17 toward the mount 22, generally
followingthe contour of the funnel wall, until it terminates in a mid-region between
the mask and mount to define aperture 47. While a further extension of the shield
would result in improved shielding, it would also present the risk of interference
with the magnetic beam deflection field produced by external deflection means (not
shown) positioned in the transition region between the funnel and the neck, as well
as actual physical interception (clipping) of the electron beams.
[0014] Referring now to
Fig. 2, the shield 31 is seen in plan view from the rear or mount end of the tube,
as viewed along the Z axis. In accordance with the conventional practice of labeling
regions of the tube as though the screened panel were the face of an analog clock,
the top, left side, bottom, and right side of the shield are labeled the 12, 3, 6
and 9 o'clock sides, respectively. As can be seen, the slots 41a and 41b are located
in the centres of the 6 and 12 o'clock sides.
[0015] The slots may also be located off-center, for example within a central region of
the 6 and 12 o'clock sides, this region defined as extending up to 40 percent of the
length La ofthe aperture. There may also be more than one slot in a sidewall, but
preferably there will be the same number of slots in each sidewall. In addition, the
facing slots need not be superjacent as shown, but may be displaced relative to one
another, within the central region defined.
[0016] The slots have a height h which is from about 50 to 95 percent of the height Hs of
the shield from the rim 48 to the straight edge 49 of the aperture 47, and a width
w which is from about 1 to 10 percent of the length Lr of the shield at the rim 48.
[0017] The aperture 47 is oblong-shaped, having a length-to-width ratio of from about 1.7
to 2.1, and having a central region defined by straight edges 49 and two end regions
defined by curved edges 50. As may be seen more clearly in Figs. 1 and 3, the central
region of the aperture lies in a plane normal to the Z axis, while the end regions
lie in upwardly curving surfaces, resulting in the curved edge profile seen in Fig.
3.
[0018] The aperture has a width Wa which is from about 49 to 51 percent of the width Wr
of the shield at the rim 48, and a length La which is from about 65 to 69 percent
of the length Lr. In addition, the amount of upward
[0019] curvature of the end regions of the aperture, resulting from the intersection of
the bowl-shaped sidewalls with the oblong-shaped aperture, is indicated by the height
He of the shield from the rim 48 to the outer point 52 of curved edge 50, and this
height Hc may range from about 85 to 90 percent of the height Hs.
[0020] Within the above ranges, the aperture has a larger length-to-width ratio than the
apertures of certain prior shield designs (about 2 versus 1.3). This change has the
effect of improving north-south shielding, but at the expense of slightly reduced
east-west shielding. East-west shielding is at least partially recovered, however,
by introducing the slots into the 6 and 12 o'clock sidewalls.
[0021] By way of example, 19V mini neck color tubes having a shield of the invention and
a prior art shield were fabricated and compared for registration differences. The
shield of the invention was as shown in the sidewalls, and an oblong-shaped aperture
with upwardly curving end regions, with the following dimensions in inches:
Hs = 4.0, Lr = 15.0, Wr = 10.9, Hc = 3.75, Wa = 5.37, La = 10.75, w = 0.3, and h =
3.9. The prior art shield had no slots and its aperture was entirely located in a
plane normal to the Z axis, and had the following dimensions:
Hs = 3.0, Lr = 15.0, Wr = 10.9, 1Ia
= 7.4 and
La = 9.6. Registrations (difference between stripe location and actual beam landing location;
also known as beam landing error) were measured on several sample tubes for each type
mf shield and averaged. Measurements were taken at the four corners ofthe screen for
each sample tube oriented successively in the west, south, east, north and west directions.
Registration differences between north and south facing orientations averaged about
0.6 mils or is less for the inventive shield versus about 1.2 mils for the prior art
hield. Registration differences between east and west facing orientations averaged
about 0.6 mils for the inventive shield versus about 0.5 mils for the prior art shield.
The significant improvement in north-south shiel-. ding at the expense of a slight
decrease in east-west shielding resulted in a beneficial correction of the effects
of external magnetic fields, and a consequent overall improvement in tube performance.
[0022] In accordance with another aspect of the invention, the shield is fabricated from
a foil sheet of soft magnetic material, such as low carbon steel. The sheet is shaped
by forcing it over a mold, resulting in simultaneously stretching and crimping it
into the desired shape. The crimps are represented in the drawings by the randomly
distributed loopedand wavy lines.
[0023] The slots are preferably formed before shaping (such as by cutting or punching) because
after shaping the slots lie in a curved surface and forming in such a surface is more
difficult than in a flat surface. Because the slots are located in an area of the
foil which undergoes considerable stretching during shaping, it is important that
the slots adhere to the dimensional and other limitations set forth herein, in order
to avoid tearing of the foil or deformation of the slots or both, during shaping.
For the same reasons, the aperture is preferably formed after shaping.
[0024] While there have been shown and described what are at present considered to be the
preferred embodiments of the invention, it will be obvious to those skilled in the
art that various changes and modifications may be made therein without departing from
the scope ofthe invention as defined by the appended Claims.
1. A color cathode ray tube comprising: an outer glass envelope of integrated face
panel, funnel and neck portions; a phosphor screen deposited on the inner surface
of the face panel, the screen comprised of an array of discrete phosphor elements;
at least one electron gun positioned in the neck for directing an electron beam to
the screen; and an aperture mask positioned adjacent the screen for directing the
beam to the desired phosphor elements on the screen; the tube having an axis of rotat-
tion designated the Z axis, and top, right side, bottom and left side surfaces surrounding
the Z axis, the surfaces (as seen by the viewer) designated the 12, 3, 6 and 9 o'clock
surfaces, respectively;
an internal magnetic shield positioned between the mask and the gun, the shield comprising
a bowl-shaped structure having arim extending around the periphery ofthe mask and
a sidewall extending from the rim rearward along the inner surface of the funnel toward
the neck, the structure terminating forward of the neck to define an aperture for
passing the beam to the mask and screen;
characterized in that the shield has at least one slot-shaped opening in both the
6 and 12 o'clock sides of the structure, each opening aligned in the direction of
the Z axis of the tube.
2. The cathode ray tube of Claim 1 in which the structure has a pair of slots, the
first opening located in the central portion of the 12 o'clock side above the Z axis,
and the second opening located in the central portion of the 6 o'clock side below
the Z axis and facing the first opening.
3. The cathode ray tube of Claim 2 in which the bbwl-shaped structure extends toward
the neck further on the 6 and 12 o'clock sides than on the 3 and 9 o'clock sides.
4. The cathode ray tube of Claim 3 in which the aperture is defined by approximately
straight 6 and 12 o'clock edges, and by outwardly and upwardly curving 3 and 9 o'clock
edges, to form an oblong-shaped aperture having a central and two side portions, the
central portion of which lies in a plane normal to the Z axis, and the side portions
of which lie in surfaces upwardly curving from the normal plane.
5. The cathode ray tube of Claim 4 in which the shield has a height from the rim to
the straight edges of the aperture Hs and a length at the rim Lr, and the slots have
a height h which is from about 50 to 95 percent of Hs, and a width w which is from
about 1 to 10 percent of La.
6. The cathode ray tube of Claim 5 in which the shield has a width at the rim Wr,
and the aperture has a width Wa which is from about 49 to 51 percent of Wr, and a
length La which is from about 65 to 69 percent of Lr.
7. The cathode ray tube of Claim 6 in which the shield has a height from the rim to
the curved edges of the aperture Hc which is from about 85 to 90 percent of Hs.
8. The cathode ray tube of Claim 1 in which the aperture has a ratio of length La
to width Wa of from about 1.7 to 2.1.
9. The cathode ray tube of Claim 8 in which the structure is comprised of a crimped
foil sheet of a soft magnetic material.
10. A method of producing an internal magnetic shield for a color cathode ray tube,
the method comprising; first forming at least one pair of slots in a foil sheet of
soft magnetic material; and then forcing the material over a bowl-shaped mold to stretch
the foil sheet into a bowl-shaped structure.
11 The method of Claim 10 in which after shaping, an aperture is formed in the structure.