FIELD OF THE INVENTION
[0001] The invention relates to a cathode ray tube comprising a panel portion with a long
axis, a short axis and a diagonal, and provided with a skirt, a funnel portion and
a neck portion comprising an electron gun for generating one or more electron beam(s),
and a deflection system mounted on said funnel portion for generating electromagnetic
fields for deflecting said electron beam(s) and a colour selection electrode.
[0002] The invention also relates to a panel portion for a cathode ray tube.
[0003] The invention also relates to a display apparatus comprising a CRT.
BACKGROUND OF THE INVENTION
[0004] Cathode ray tubes (CRT's) of the type described in the opening paragraph are known.
An example is given in US 6,274,977.
In such tubes the colour selection electrode is often also called a shadow mask.
[0005] The cathode ray tubes have to meet a number of sometimes conflicting conditions.
They have to be strong for safety reasons, provide a good image, i.e. provide an image
of high quality, be cheap, and have a nearly flat front. Although every one of these
conditions is relatively easily obtainable, it is very difficult to provide for a
cathode ray tube which meets all or most such requirements simultaneously, i.e. provide
a good balance between costs and quality.
SUMMARY OF THE INVENTION
[0006] It is an object of the invention to provide a cathode ray tube of the type described
in the opening paragraph which does provide a good balance between costs and quality.
[0007] To this end the cathode ray tube is characterized in that the color selection electrode
is made of a material with a high thermal expansion coefficient and in that the panel
portion has the following features:
- an outside radius of curvature of more than 30000 mm
- wherein the following relations hold
- 0.85≤Ts/Td≤1
- 0.6≤Tl/Td≤0.72
- 0.67≤Tc/Td≤0.34
- wherein Tc is a glass thickness at the centre of the front portion
- Ts is a glass thickness at the end of the short axis, at the end of the effective screen
area
- Tl is a glass thickness at the end of the long axis, at the end of the effective screen
area
- Td is a glass thickness at the end of the diagonal, at the end of the effective screen
area.
As explained above the cathode ray tube has to meet several partially conflicting
conditions. The use of a color selection electrode made of a material with a high
thermal expansion coefficient is cost effective. The high value for the outside radius
of curvature gives a nearly flat appearance to the front of the cathode ray tube.
The difference in glass thicknesses T
c, T
s, T
l and T
d allow for a relatively strong front portion. The ratios of the various thicknesses
determine the inner radii of curvature of the panel portion. These ratios influence
the radii of curvature of the color selection electrode and the intensity variations
of the image seen by a viewer. Generally it holds that the greater the curvature of
the color selection electrode, the stronger the color selection electrode becomes
and the less susceptible it becomes to doming, microphony and drop test. It also holds
that the greater the curvature of the color selection electrode, in general the larger
the variations in image intensity.
[0008] The inventor has realized that the indicated ranges of ratios of curvature on the
inner side of the panel portion allow in particular the doming behavior to be considerably
improved in relation to known devices having a color selection electrode with a high
thermal expansion coefficient, thus providing an improvement in image quality, while
in relation to devices having a color selection electrode made of a material with
a small thermal expansion coefficient, considerable cost savings (approximately 10%
of total costs of the CRT) are obtained while yet preserving a high standard in image
quality. Thus the cathode ray tube of the invention provides, in relation to prior
art devices, a better balance between costs and quality. Surprisingly the quite considerably
thickness variations of the glass, which prima facie one could imagine to have a "rounding"
effect on the image as perceived by the viewer, do not noticeably negatively influence
the overall flatness impression of the image, as long as the curvature on the outside
of the front portion is small. A material having a large thermal expansion coefficient
has a thermal expansion coefficient of larger than 5 10
-6 °C
-1. An example of such a material is Akoca steel having athermal expansion coefficient
of 11.7 10
-6 °C
-1, an example of a material having a low thermal expansion coefficient is Invar with
a thermal expansion coefficient of approximately 1.2 10
-6 °C
-1.
[0009] In preferred embodiments the following relation holds: 0.5≤T
c/T
d≤0.34.
Within this range the best conditions are obtained.
[0010] Preferably the aspect ratio of the cathode ray tube is 3:4
[0011] These and other aspects of the invention are apparent from and will be elucidated
with reference to the embodiments described hereinafter.
BRIEF DESCRIPTION OF THE DRAWINGS
[0012] In the drawings:
Fig. 1 illustrates a cathode ray tube and a picture display device in accordance with
the invention.
Fig. 2 shows a front panel of a cathode ray tube.
Fig. 3 shows a panel portion.
Fig. 4 illustrates in a graphical form the various relationships between thicknesses
in accordance with the invention.
[0013] The figures are not drawn to scale. Generally, identical components are denoted by
the same reference numerals in the figures.
[0014] A cathode ray tube and a picture display device according to a preferred embodiment
of the invention is shown in FIG.1.
[0015] It comprises a cathode ray tube 1, which includes a panel portion, sometimes also
called a display window 2, a funnel portion 3, and a neck portion 4 (or neck as it
is called hereinbelow). In the neck 4, there is as a means 5 for generating electron
beam(s) in this example three in-line electron beams 6, the in-line plane being parallel
to the long axis of the display screen, such means are herewithin in short described
by the word "electron gun". A means for generating an electron beam is usually an
in-line electron gun. Such designs are standard designs. The inner surface of the
panel portion 2 comprises a large number of phosphor elements which form a display
screen 8. When one or more of the electron beams 6 hit phosphor elements, the latter
become phosphorescent, thereby creating a visible spot on the display screen 8. In
the undeflected state, the middle one of the electron beams 6 substantially coincides
with the tube axis 7. The direction of the tube axis is hereinbelow denoted by the
z-direction. The direction along the long axis of the display screen is denoted by
the x-direction, the direction along the short axis of the display screen by the y-direction.
The line scanning direction (i.e. the direction in which scanning with the highest
frequency takes place is usually parallel to the long axis (the x-direction) of the
display screen. On its way to the display screen 8, the electron beams 6 are deflected
by means of a deflection system 9 covering a part of the funnel portion 3. It is in
particular this part 3a of the outer contour that the invention relates to. Said deflection
system 9 comprises a line deflection subsystem 12 and a frame deflection subsystem
13, in order to create a two-dimensional picture on the display screen 8. In this
exemplary embodiment, the deflection system 9 is made up of sets of coils, one set
for the line deflection subsystem 12 and another set for the frame deflection subsystem
13. The figure shows an in-line CRT, having a shadow mask 14. The electron beams pass
apertures in the shadow mask 14 before they hit the screen 8. A large percentage of
the electrons are absorbed by the shadow mask which consequently is raised in temperature.
Differences in intensity of the electron beams lead to local differences in temperature,
which lead to local distortions of the shadow mask so-called doming. These doming
distortions lead to image flaws.
[0016] The figure also indicates the x-direction, i.e. the direction along the long axis
of the display screen and the z-direction. The z-coordinate of the deflection plane
is usually (and hereinbelow) taken to be zero, with positive values of z being closer
to the display screen.
[0017] As can be seen from FIG. 2, the panel portion (8) has an elongated shape with two
perpendicular axes of symmetry : a long axis whose length, measured from screen end
to screen end, is L
scr and a short axis whose length is S
scr. Often the short axis is the vertical axis, the long axis is the horizontal axis.
In order to quantify the amount of elongation of the display screen (8), the aspect
ratio of the display screen (8) is defined as A
scr = L
scr/S
scr. The diagonal, measured from screen comer to an opposite screen comer has a length
D wherein approximately D
2= L
2scr + S
2scr. The panel portion comprises an upstanding wall 21 and a front part 22. Figure 2
also shows the maximum deflection angle Θ as being the angle between the tube axis
(7) and the deflected electron beam (10) when the electron beam is deflected so as
to hit a point on the display screen which is the furthest away from the intersection
between the tube axis (7) and the display screen.
[0018] The following relation holds

[0019] Depending on the design A
scr is usually 3/4 or 9/16. In preferred embodiments the aspect ratio is ¾.
The outer side of the panel portion is nearly flat, i.e. it has an outside radius
of curvature R of more than 30000 mm (30 m). If there are more than one radii of curvature,
for instance vertically and horizontally each of the radii of curvature has a value
of more than 30000 mm. Preferably all radii of curvature are larger than 40000 mm.
Preferably the outside radius is less than 100000 mm (100 m). For nearly completely
flat front surfaces sometimes shows hollow impressions.
The thicknesses of the panel portion, except for the centre glass thickness are taken
at the end of the screen
The following thicknesses are of importance:
Tc, the glass thickness at the centre of the front portion,
Ts, the glass thickness at the end of the short axis Sscr,
Th is a glass thickness at the end of the long axis Lscr,
Td is a glass thickness at the end of the diagonal D.
[0020] The ratios between these thicknesses are, for cathode ray tubes in accordance with
the invention set between:
- 0.85≤Ts/Td≤1
- 0.6≤Th/Td≤0.72
- 0.67≤TcTd≤0.34
[0021] The invention is based on the following insights:
[0022] The thickness variations of the panel portion are set between the indicated limits.
This strengthens the shadow mask and makes it less susceptible for doming. Use is
made of a shadow mask of high thermal expansion coefficient. A considerable reduction
in prize, compared to devices using a shadow mask with a small thermal expansion coefficient,
while yet preserving high image quality is obtained.
Surprisingly the quite considerably thickness variations of the glass, which prima
facie one could imagine to have a "rounding" effect on the image as perceived by the
viewer, do not noticeably negatively influence the overall flatness impression of
the image, as long as the curvature on the outside of the front portion is small,
i.e. radius R is large. Even larger inner radii of curvature (i.e. ratios outside
the indicated ranges), do, however, lead to a visual effect on the image, reducing
the sought-after flat image effect. So the cathode ray tube in accordance with the
invention pairs a flat image reproduction, to a cost reduction, while yet preserving
image quality, in particular reducing doming errors. Doming constitutes for color
selection electrodes made of a material with a high thermal expansion coefficient,
and such in contrast to color selection electrodes made of a material with a small
thermal expansion (such as Invar), a serious problem with a serious detrimental effect
on image quality.
[0023] It is remarked that the curvature of the front part is grossly exaggerated in this
figure. Figure 3 illustrates in more detail a panel portion. The thicknesses are taken
at the end of the screen area, i.e. where the phosphor layer ends.
[0024] Figure 4 illustrates in a graphical form the ranges for the ratios. Indicated are
the ratios in accordance with the invention, as well as for the ratio T
c/T
d for preferred embodiments. Indicated in this figure are also, for easy reference,
the ratios mentioned in US 6,274,977, by means of the dotted lines. There are clear
differences in the ratios, furthermore, US 6,274,977 does not discuss the material
for the shadow mask. Despite the fact the US 6,274,977 mentions that thickness ratios
T
l/T
d would lead to a shadow mask of inadequate strength, the inventors have realized that
using a shadow mask of a material having a high thermal expansion coefficient, it
is possible to maintain adequate structural strength, while yet maintaining good image
reproduction, in particular having good doming behavior, and reducing costs in respect
of using a shadow mask of a material having a low thermal expansion coefficient. In
an example, a 21" CRT with an aspect ratio of 3/4 the value for T
s/T
d was 0.88, the value for T
l/T
d was 0.67 and the value for T
c/T
d was 0.41. For a 25" CRT the values are 0.88, 0.67 and 0.40 respectively.
[0025] The invention is particular useful for CRT's in the range between 20" and 27".
[0026] In short the invention may be described as follows:
A cathode ray tube (1) comprises an panel portion (2), a funnel portion (3) and a
neck portion (4) with an electron gun (5) and a shadow mask. The shadow mask is made
of a material with a high thermal expansion coefficient, and the panel portion has
an outside radius of curvature (R) larger than 30000 mm. The thicknesses of the panel
portion have the following ratios:
0.85≤Ts/Td≤1
0.6≤Tl/Td≤0.72
0.67≤Tc/Td≤0.34
wherein T
c is a glass thickness at the centre of the front portion
T
s is a glass thickness at the end of the short axis, at the end of the effective screen
area
T
l is a glass thickness at the end of the long axis, at the end of the effective screen
area
T
d is a glass thickness at the end of the diagonal, at the end of the effective screen
area.
[0027] It will be clear that within the concept of the invention many variations are possible.
It will be appreciated by persons skilled in the art that the present invention is
not limited by what has been particularly shown and described hereinabove. The invention
resides in each and every novel characteristic feature and each and every combination
of characteristic features. Reference numerals in the claims do not limit their protective
scope. Use of the verb "to comprise" and its conjugations does not exclude the presence
of elements other than those stated in the claims. Use of the article "a" or "an"
preceding an element does not exclude the presence of a plurality of such elements.
1. A cathode ray tube (1) comprising a panel portion (2) with a long axis, a short axis
and a diagonal, a funnel portion (3) and a neck portion (4) comprising an electron
gun (5) for generating one or more electron beam(s) (6), and a deflection system (9)
mounted on said funnel portion (3) for generating electromagnetic fields for deflecting
said electron beam(s) (6), and a color selection electrode (14)
characterized in that the color selection electrode (14) is made of a material with a high thermal expansion
coefficient and
in that the panel portion (2) has the following features:
• an outside radius of curvature (R) of more than 30000 mm
• wherein the following relations hold
• 0.85≤Ts/Td≤1
• 0.6≤Tl/Td≤0.72
• 0.67≤Tc/Td≤0.34
• wherein Tc is a glass thickness at the centre of the front portion
• Ts is a glass thickness at the end of the short axis, at the end of the effective screen
area
• Tl is a glass thickness at the end of the long axis, at the end of the effective screen
area
• Td is a glass thickness at the end of the diagonal, at the end of the effective screen
area.
2. A cathode ray tube as claimed in claim 1, wherein 0.5≤Tc/Td≤0.34.
3. A cathode ray tube as claimed in claim 1 or 2, wherein the outside radius of curvature
(R) is less than 100000 mm.
4. A cathode ray tube as claimed in any of the preceding claims wherein the aspect ratio
is substantially 3/4.
5. A panel portion (2) for a cathode ray tube with a long axis, a short axis and a diagonal,
a funnel portion (3) and a neck portion (4)
characterized in that the panel portion (2) has the following features:
• an outside radius of curvature (R) of more than 30000 mm
• wherein the following relations hold
• 0.85≤Ts/Td≤1
• 0.6≤Tl/Td≤0.72
• 0.67≤Tc/Td≤0.34
• wherein Tc is a glass thickness at the centre of the front portion
• Ts is a glass thickness at the end of the short axis, at the end of the effective screen
area
6. A panel portion as claimed in claim 5, wherein the panel portion has an aspect ratio
of 3/4.
7. A panel portion as claimed in claim 5 or 6 wherein the outside radius of curvature
is less than 100000 mm.
8. A display apparatus comprising a cathode ray tube as claimed in any of the claims
1 to 4.