Technical Field
[0001] The present invention relates to a variable color lamp with a dimmer function.
Background Art
[0002] When a light source includes a number of lamps with different luminous colors, the
color of the light emitted from the source is varied by switching over the lamps.
[0003] Several devices have been proposed for continuously changing the chromaticity of
light emitted from a discharge lamp; for example, Japanese Patent Publication Gazette
No. Sho-53-42386 and Japanese Patent Laying-Open Gazette No. Sho-63-198295. In such
devices, gas or vapor sealed in a discharge lamp as a luminescent material varies
its luminous color corresponding to the intensity of electronic energy, that is, the
waveform of a pulse, in the discharge lamp. When the ratio of power supplying time
to idle period is relatively large, the color of the light emitted from the lamp is
blue; on the other hand, when the ratio is relatively small, the color of the light
emitted from the lamp is red.
[0004] The former method, however, requires a large number of luminous lamps corresponding
to various colors and therefore makes a device bulky. Such a device occupies large
space and is not suitable for private purposes, that is, lighting in or out of the
houses or illumination at shop windows.
[0005] In the latter method, on the other hand, since a longer idle period is required for
red light emission, power supplied to the discharge lamp becomes rather small and
luminance of the light may be insufficient for illumination.
[0006] The objective of the invention is thus to provide a space-saving variable color lamp
which emits light of various chromaticity and sufficient luminance.
Disclosure Invention
[0007] The invention attains the foregoing and other objectives with a variable color lamp
with a dimmer function, which includes: plural emission tubes each emitting light
of different chromaticity; and control means for regulating power supplied to each
of the plural emission tubes.
[0008] Power supplied to each of the emission tubes is regulated by the control means, and
each emission tube emits light of self-luminous color corresponding to the power.
[0009] The variable color lamp of the invention occupies smaller space than the conventional
light source including a large number of lamps with different luminous colors. The
color lamp of the invention does not require idle period for light emission of any
color or tint and can thus emit light of neutral tints with sufficient luminance.
[0010] The simple structure of the invention attains light emission of a wide range of color
variation at relatively low cost.
[0011] The control means includes a relative output control unit for varying the relative
output or the quantity of light emitted from each of the plural emission tubes. The
variable color lamp of the invention thus emits light of a neutral tint according
to the relative outputs of the plural emission tubes. Namely, the luminous color of
the lamp is varied corresponding to color matching functions of chromaticity coordinates.
[0012] In another aspect, the invention comprises a variable color lamp including: a first
emission tube for emitting blue light of a first wavelength range; a second emission
tube for emitting green light of a second wavelength range; and a third emission tube
for emitting red light of a third wavelength range.
[0013] The color lamp of the invention has the three emission tubes each discharging light
of one of the additive primaries proper to the tube, thus attaining a wider color
variation and reproducing the color of irradiated objects vividly.
[0014] The first through the third emission tubes are all discharge tubes; the first emission
tube includes indium halide sealed therein; the second emission tube includes thallium
halide sealed therein; and the third emission tube includes sodium halide sealed therein.
[0015] In the variable color lamp including the first through the third emission tubes each
emitting light of one of additive primaries proper to the tube or discharging color
light determined by the metal halide sealed in the tube, the first through the third
emission tubes are arranged adjacent to and parallel to one another.
[0016] The three emission tubes may be arranged in parallel on the same plane such that
the first emission tube is placed in between the second and the third emission tubes.
The emission tube disposed in the middle is the first emission tube with indium halide
sealed therein which has a narrow dimmer range than thallium halide or sodium halide.
[0017] The three emission tubes disposed adjacent to and parallel to one another or arranged
in parallel on the same plane in the predetermined order may be integrally formed
in the variable color lamp of the invention. Such structure enables the adjacent emission
tubes to transfer thermal energy generated from the tubes to each other and to attain
uniform temperature rise. Each emission tube thus reaches stable lighting conditions
within a short time period.
[0018] The emission tube disposed in the middle receives thermal energy generated from both
the side tubes. Namely, the middle tube with indium halide receives thermal energy
from both the adjacent emission tubes and is thereby maintained at high temperature.
[0019] This structure of the invention attains a wider range of color variation of the emission
tubes as described below.
[0020] A high intensity discharge lamp including one emission tube generally has a dimmer
range of approximately ten percent. The dimmer range of the discharge lamp is narrower
than incandescent lamps and tungsten halogen lamps because of the following reasons.
In the high intensity discharge lamp, when input to the emission tube is limited in
order to decrease the light flux, the temperature in the emission tube is lowered
and the luminescent material such as In (indium), Tl (thallium), or Na (sodium) sealed
in the emission tube varies its partial vapor pressure. When the partial vapor pressure
drops down to a predetermined threshold or lower value, the lamp does not discharge
any light but is in 'OFF' state. In the conventional high intensity discharge lamp
with only one emission tube, the possible dimmer range is within approximately ninety
percent of the rated output.
[0021] In the variable color lamp of the invention, on the other hand, plural emission tubes
are disposed adjacent to and parallel to each other, and thermal energy generated
from each emission tube is transferred to the other emission tubes through the common
side wall of the tubes. Even when input to one emission tube is limited, thermal energy
generated from the adjacent emission tubes is given to that one tube. Accordingly
the emission tube with limited input in the structure of the invention is maintained
at higher temperature than the only one emission tube with limited input in the conventional
high intensity discharge lamp. The partial vapor pressure of the luminescent material
sealed in the emission tube with limited input does not vary but is kept relatively
constant, so that the possible dimmer range of the emission tube becomes wider.
[0022] Input to one emission tube may be decreased while input to the other two emission
tubes is increased. This allows the total input to the whole variable color lamp to
be kept constant and thereby prevents the temperature fall of the emission tube with
limited lower input so as to attain a wider dimmer range.
[0023] The variable color lamp of the invention can emit light of a wider chromaticity range
corresponding to the wider dimmer range of the emission tube.
[0024] In the variable color lamp of the invention, the emission tube disposed in the middle
contains indium halide emitting bluish purple line spectrum and having a relatively
narrow dimmer range. Thallium halide emitting green line spectrum and having a relatively
wide dimmer range and sodium halide emitting reddish orange line spectrum and having
a relatively wide dimmer range are respectively sealed in the side emission tubes
arranged in parallel with the middle tube.
[0025] When input to the middle emission tube with indium halide having a relatively narrow
dimmer range is decreased and the same to the side emission tubes with thallium halide
or sodium halide having a relatively wide dimmer range is increased, thermal energy
generated from the side tubes is transferred to the middle emission tube so as to
maintain the middle tube at high temperature. The possible dimmer range of the middle
emission tube is thus made wider than the original dimmer range of the sealed luminescent
material.
[0026] The plural emission tubes of the invention are composed of translucent alumina ceramics
prepared by sintering fine powdery alumina of at least 99.99 mol% in purity. The average
grain diameter of the translucent alumina particles is not greater than one micrometer
and the maximum grain diameter is not greater than two micrometer.
[0027] Since high purity of alumina does not virtually form the grain boundary phase, the
emission tube of translucent alumina ceramics has improved mechanical strength (bending
strength and Weibull coefficient) at ambient to discharge temperatures, compared with
an emission tube of conventional translucent ceramics prepared by sintering and growing
grains with a sintering accelerator such as MgO. The improved mechanical strength
allows the emission tube to have thinner wall and thereby smaller thermal capacity.
Accordingly the luminous part of the emission tube is heated to a predetermined temperature
at a high speed and warm-up time of the tube is shortened. Here the warm-up time represents
a time period until discharging metal component (metal halide) sealed in the tube
vaporizes to saturated vapor pressure.
[0028] The emission tube may be any discharge tube with high lamp efficacy; for example,
metal halide tubes, high-pressure sodium tubes, and fluorescent tubes.
[0029] Japanese Industrial Standard JIS Z8110 defines the relationship between the self-luminous
color of a monochromatic light source and the wavelength range as follows:
380 to 455 nm: bluish purple
455 to 485 nm: blue
485 to 495 nm: blue green
495 to 548 nm: green
548 to 573 nm: yellow green
573 to 584 nm: yellow
584 to 610 nm: reddish orange
610 to 780 nm: red
[0030] In the invention, the wavelength range of blue light denotes 380 to 495 nm; the wavelength
range of green light represents 485 to 573 nm; and the wavelength range of red light
is 573 to 780 nm.
Brief Description Of Drawings
[0031]
Fig. 1 is a vertical cross sectional view showing a variable color lamp of a first
embodiment according to the invention;
Fig. 2 is an x-y chromaticity diagram showing the relationship between the relative
output of an emission tube and the luminous color in the variable color lamp of the
first embodiment;
Fig. 3 is a block diagram showing the electric structure of the variable color lamp
of the first embodiment;
Fig. 4 is a perspective view illustrating an emission tube 1M built in a variable
color lamp according to a second embodiment;
Fig. 5 is a process chart showing manufacturing process of the emission tube 1M;
Fig. 6 is a perspective view illustrating another emission tube 1N;
Fig. 7 is a graph showing distribution of the grain diameter of translucent alumina
constituting the emission tube 1M;
Fig. 8 is a perspective view illustrating another emission tube 1L applied to modification
of the second embodiment;
Fig. 9 is a perspective view illustrating another emission tube 1R applied to modification
of the second embodiment and a mold used for manufacturing the tube 1R;
Fig. 10 is a perspective view illustrating another emission tube 1S applied to modification
of the second embodiment;
Fig. 11(a) is a perspective view illustrating another emission tube 1A used in place
of the emission tubes 1R and 1S;
Fig. 11(b) is a Y-plane cross sectional view of Fig. 11(a);
Fig. 12 is a process chart showing manufacturing process of the emission tube 1A;
Figs. 13(a) and 13(b) are perspective views showing a mold used in manufacture of
the emission tube 1A;
Fig. 14 is an explanatory view illustrating manufacture of the emission tube 1A; and
Fig. 15 is an explanatory view also illustrating manufacture of the emission tube
1A.
Best Mode for Carrying Out the Invention
[0032] Preferred embodiments of the invention are hereinafter described in detail according
to the drawings.
[0033] Fig. 1 is a vertical cross sectional view showing a variable color lamp of a first
embodiment according to the invention.
[0034] A variable color lamp 1 includes a first emission tube 3, a second emission tube
4, and a third emission tube 5 via a support 15 in an outer bulb 2 having a reflector
mirror 17 on the upper side thereof. The outer bulb 2 is composed of a translucent
material having light scattering ability, for example, frosted glass, milky glass
or acrylic resin. Metal halide (luminescent material) for emitting light of a different
luminous color is sealed with mercury and starting noble gas in each of the emission
tubes 3 through 5. A pair of primary electrodes 6 and 9, 7 and 10, or 8 and 11 are
adhered to either end of the emission tube via molybdenum foils. Auxiliary starting
electrodes 12, 13, and 14 are also fixed to the lower end of the emission tubes, respectively.
The primary electrodes and the auxiliary starting electrodes are connected to a power
control circuit 20 (described later) through pins 16.
[0035] The emission tubes 3 through 5 are composed of quartz glass, and the primary electrodes
mounted on both the ends of the emission tube are coils of tungsten and the like.
The outer bulb 2 may be evacuated or filled with gas.
[0036] The first emission tube 3 contains indium halide such as InI₃ with mercury and starting
noble gas, and emits bluish purple line spectrum at the wavelength around 411 nm or
451 nm. The second emission tube 4 contains thallium halide such as TlI with mercury
and starting noble gas, and emits green line spectrum at the wavelength around 535
nm. The third emission tube 5 contains sodium halide such as NaI with mercury and
starting noble gas, and emits reddish orange line spectrum at the wavelength around
589 nm.
[0037] Fig. 2 is an x-y chromaticity diagram showing the relationship between the relative
output of the emission tube and the luminous color. In the diagram, points A, B, and
C represent luminous colors of the emission tubes 3 through 5, respectively. The luminous
color of the variable color lamp 1 may be varied within a triangle of the three points
A, B, and C in conformity with the rule of color addition (the additive mixture of
colors). For example, when outputs of the second and the third emission tubes 4 and
5 are set greater than that of the first emission tube 3, the luminous color of light
emitted from the variable color lamp 1 is pale yellowish green shown by a point D.
[0038] The electric structure of the variable color lamp 1 of the first embodiment is explained
based on the block diagram of Fig. 3. The auxiliary starting electrodes are omitted
in the diagram since they are not essential for the scope of the invention.
[0039] The power control circuit 20 includes three dimmers 21, 22, and 23 and three ballasts
24, 25, and 26 corresponding to the three emission tubes 3, 4, and 5. The dimmers
21 through 23 are semi-conductor phase control circuits connected to an AC power source
18 in series. When the emission tubes 3 through 5 have different rated voltages, each
dimmer may be connected to an individual AC power source for applying a different
rated voltage.
[0040] A color control circuit 30 includes an input area 31, an output distribution calculator
32, an emission tube output calculator 33, and three dimmer signal output areas 34,
35, and 36.
[0041] A remote control unit 40 includes a chromaticity setting area 42 and a lamp output
setting area 43. The remote control unit 40 has a series of keys for inputting commands
and a display for showing operation of the lamp.
[0042] The luminous color or the light flux of the lamp may be varied by setting the chromaticity
and output of the lamp through the keys of the remote control unit 40. The chromaticity
is, for example, input as coordinate values on the x-y chromaticity coordinates. The
coordinates of the point D in Fig. 2 are (0.37, 0.45) in the x-y chromaticity coordinate
system. The output of the lamp is, for example, input as a percentage relative to
the maximum output of the lamp at each chromaticity. The chromaticity setting area
42 and the lamp output setting area 43 of the remote control unit 40 respectively
generate a chromaticity signal Sc and a lamp output signal Sp corresponding to the
input values, and transfer data to the input area 31 of the color control circuit
30.
[0043] The chromaticity signal Sc is sent from the input area 31 to the output distribution
calculator 32, which determines the relative value of the total luminous flux emitted
from each of the three emission tubes 3 through 5 according to the additive mixture
of colors so as to attain the chromaticity shown by the chromaticity signal Sc.
[0044] The emission tube output calculator 33 determines the output level of each emission
tube based on the relative value of the total luminous flux, that is, the relative
output, of the emission tube determined by the output distribution calculator 32 and
the lamp output signal Sp. The output level of the emission tube having the maximal
relative output determined by the output distribution calculator 32 is set equal to
a value multiplying the rated output of the emission tube by the relative output (percent)
shown by the lamp output signal Sp. For example, when the relative output values of
the three emission tubes are 0.6: 0.4: 1.0 and the relative output of the lamp output
signal Sp is seventy percent, the output levels of the emission tubes are respectively
set to 42%, 28%, and 70%.
[0045] Signals representing the output levels of the emission tubes are sent from the emission
tube output calculator 33 to the three dimmer signal output areas 34 through 36, which
generate dimmer signals (fade signals) for controlling the dimmers 21 through 23.
Each of the dimmers 21 through 23 controls a continuity phase angle of current supplied
to the emission tube corresponding to the dimmer signal output from the dimmer signal
output area 34, 35, or 36. Current running through the emission tube and the total
luminous flux of the emission tube are thus adjusted. Since the efficiency of the
emission tube varies with the current, the total luminous flux is not always proportional
to the feed quantity. The emission tube output calculator 33 corrects the signals,
which are sent to the dimmer signal output areas 34 through 36, with a predetermined
calibration curve according to the relationship between the total luminous flux of
the emission tube and the feed quantity, such that the ratio of the output signals
is equal to the ratio of the total luminous fluxes of the emission tubes determined
by the output distribution calculator 32.
[0046] The emission tubes 3 through 5 are installed in the outer bulb 2 composed of a translucent
material with light scattering function, for example, frosted glass, milky glass or
acrylic resin. Mixing failure of the luminous fluxes of the plural colors due to misalignment
of the emission tubes is hence well prevented by the blurring of such a translucent
material.
[0047] The variable color lamp 1 of the first embodiment includes three emission tubes each
discharging color light similar to one of additive primaries, that is, Red, Green,
and Blue. The luminous color of the variable color lamp 1 is adjustable within almost
the whole visible light on the x-y chromaticity diagram by varying the relative outputs
of the emission tubes. Namely, the luminous color of the lamp is varied corresponding
to color matching functions of the chromaticity coordinate system. The line spectra
of the emission tubes are also close to the additive primaries , and the color of
an irradiated object is thereby reproduced vividly.
[0048] The emission tubes 3 through 5 of the variable color lamp 1 may be any discharge
tube such as incandescent tubes, fluorescent tubes, high-pressure sodium tubes, and
neon tubes as well as the metal halide tubes used in the first embodiment. For example,
when a neon tube emitting red line spectrum is used for the third emission tube 5
(the metal halide tube containing sodium halide such as NaI in the first embodiment),
wider color variation is implemented.
[0049] Emission tubes emitting continuous spectrum may be used in place of those with line
spectrum in a certain wavelength range.
[0050] In another aspect, certain additives may be mixed with alumina to give specific spectral
characteristics to the translucent alumina emission tube with hydrogen, iodine, and
starting noble gas sealed therein. When chromium compound is added to alumina, red
line spectrum is obtained; cobalt compound for blue line spectrum; and nickel or zinc
compound for green line spectrum. The specific spectral characteristics may be attained
by coloring the whole emission tube or forming a colored layer on the surface of the
emission tube. In the first method, solid solution of the metal oxide (additive) is
mixed with alumina while translucent alumina is sintered. In the latter method, on
the other hand, solid solution of the metal oxide is painted on the circumference
of the alumina emission tube.
[0051] The number of the emission tubes is determined according to the requirement. Two
emission tubes are, for example, used when the coloring range is a line, while four
tubes are used when a wider band range should be covered.
[0052] Another variable color lamp of a second embodiment according to the invention is
described hereinafter. In the following description, members having the same functions
as the first embodiment may not be explained, nor may symbols or numerals assigned
to such members be omitted.
[0053] In the first embodiment, the three emission tubes 3 through 5 are independently installed
in the outer bulb. The second embodiment, on the other hand, includes an emission
tube 1M consisting of three emission pipes integrally formed in parallel on the same
plane as shown in Fig. 4.
[0054] The emission tube 1M, composed of translucent alumina, is a multi-pipe tube consisting
of three single emission pipes 1m1, 1m2, and 1m3 which are integrally formed adjacent
to and parallel to one another. Each emission pipe has a pair of primary electrodes
and generates linear electric discharge space. The side wall of the single emission
pipes 1m1 and 1m2 or 1m2 and 1m3 is in common as indicated by shaded parts in Fig.
4.
[0055] The inner diameter of each single emission pipe 1m1, 1m2, and 1m3 ('d' in Fig. 4)
is approximately 4.0 mm, and the wall thickness ('d0' in Fig. 4) is about 0.2 mm.
The distance between the primary electrodes adhered in each emission pipe is approximately
30 mm.
[0056] Manufacture of the emission tube 1M is described according to the process chart of
Fig. 5.
[0057] Fine powdery alumina, material of the emission tube 1M is first synthesized. Aluminum
salt, which gives at least 99.99 mol% in purity of alumina by pyrolysis, is used as
a starting material. Examples of such aluminum salt for yielding high purity of alumina
include ammonium alum and aluminum ammonium carbonate hydroxide (NH₄AlCO₃(OH)₂).
[0058] The aluminum salt is weighed, mixed with distilled water and a dispersing agent to
a suspension, and dried by spray drying. The dried salt is then pyrolyzed to fine
powdery alumina at the temperature between 900 and 1200°C, for example, 1050°C, in
the atmosphere for two hours. Through the process of spray drying and pyrolysis, fine
powdery alumina (average grain diameter: 0.2 to 0.3 micrometer, purity: at least 99.99
mol%) is prepared. Secondary aggregate of alumina fine powder, which has a greater
diameter than the powder, is actually yielded.
[0059] An organic binder mainly consisting of acrylic thermoplastic resin is mixed with
the secondary aggregate of alumina fine powder. The mixture in an organic solvent
such as benzene is wet stirred with a plastic or nylon ball mill for approximately
twenty-four hours, so that the organic binder and alumina fine powder are sufficiently
wet. The mixture is then evaporated for removal of the solvent and kneaded to yield
a compound of a desired viscosity (50,000 to 150,000 cps) (process 1).
[0060] The organic binder consists of acrylic thermoplastic resin, paraffin wax, and atactic
polypropylene, and the total quantity of the binder is 25 g with respect to 100 g
of alumina fine powder.
[0061] The content of each component of the organic binder is as follows:
Acrylic thermoplastic resin: 20 to 23 g
(preferably 21.5 g)
Paraffin wax: not greater than 3 g
(preferably 2.0 g)
Atactic polypropylene: not greater than 2 g
(preferably 1.5 g)
Here, the total of the contents should be 25 g.
[0062] The mixture is evaporated at 130°C for twenty four hours and kneaded at 130°C with
an alumina roll mill to yield a compound.
[0063] The compound is injected into a cavity of a mold on an injection molding device (not
shown) and molded to a multi-pipe body W0, shown in Fig. 4, consisting of three cylindrical
emission pipes integrally formed adjacent to and parallel to one another (process
2). The compound is previously heated to 130 to 200°C (preferably 180°C), and then
injected from a nozzle of an injection device under the pressure of 900 to 1,800 kg/cm².
[0064] The compound is solidified in the injection cavity to the molded body W0 under the
certain pressing conditions; the pressure of 180 to 800 kg/cm² is kept for 0.5 to
5 seconds. The molded body W0 thus obtained has 0.99 or higher transferability (dimensions
of the molded body / those of the mold), 0.99 or higher circularity, and 0.99 or higher
contraction ratio (in the direction of the diameter / that of the axis). The inner
diameter of each cylindrical pipe of the molded body W0 is determined to be approximately
4.85 mm by considering volume shrinkage on sintering. The wall thickness ('d0' in
Fig. 4) of each cylindrical pipe is set to be approximately 0.3 mm by considering
volume shrinkage on sintering and grinding margin.
[0065] After completion of the injection molding process (process 2), the molded body W0
is parted from the mold on the injection molding device (process 3).
[0066] The molded body W0 is heated in nitrogen atmosphere to a temperature at which the
organic binder containing acrylic thermoplastic resin is pyrolyzed and completely
carbonated. Namely, the molded body W0 is degreased (process 4). The upper limit of
the heating temperature in this initial heat treatment is determined according to
the performance of the heat treatment furnace and the pyrolytic temperature of the
organic binder. In this embodiment, the molded body W0 is heated from the room temperature
(20°C) to 450°C for seventy-two hours. The conditions of the initial heat treatment
are as follows:
Pressure: 1 to 8 kg/cm²
(optimal pressure is 8 kg/cm²)
Time period for heating from 20°C to 450°C: not longer than seventy-two hours.
Here, the pressure is kept constant during heating up to 450°C.
[0067] The organic binder of acrylic thermoplastic resin, paraffin wax, and atactic polypropylene
mixed in the compound is pyrolyzed and carbonated through this initial heat treatment,
so that the molded body W0 is sufficiently degreased.
[0068] The degreased body W0 is again applied to heat treatment in the atmosphere so as
to be sintered (process 5). The conditions of the secondary heat treatment are given
below; here the heating rate is 100°C / hour:
Temperature: 1,200 to 1,300°C
(optimum temperature: 1,235°C)
Time period of treatment at the above temperature:
zero to four hours (optimum time period: two hours)
The sintering temperature is set in the range of 1,200 to 1,300°C so as to make
the actual density of the sintered body not less than 95% of the theoretical density
for the following hot isostatic pressing and prevent growth of undesirable rough crystals.
When the temperature is 1,200°C or lower, the density of the sintered body drops to
the level unsuitable for hot isostatic pressing, that is, less than 95% of the theoretical
density. When the temperature is, on the other hand, over 1,300°C, formation of rough
crystals decreases the strength of the sintered body.
[0069] Through the initial and secondary heat treatment for degreasing and sintering, the
volume of the molded body is shrunk to 82.5%, and the packing factor of the sintered
body becomes approximately 100% (bulk density: 3.976). Carbides produced in the process
of the initial heat treatment are completely burned out and removed from the sintered
body through the sintering process.
[0070] The sintered body is exposed to hot isostatic pressing in argon atmosphere or the
atmosphere of argon with oxygen of not greater than 20vol% (process 6). The conditions
of the hot isostatic pressing are given below; here the heating rate is 200°C / hour:
Temperature: 1,200 to 1,250°C
(optimum temperature: 1,230°C)
Pressure: 1,000 to 2,000 atm
(optimum pressure: 1,000 atm)
Time: one to four hours (optimum time: two hours)
The sintered body acquires translucency through this process, and the multi-pipe emission
tube 1M of translucent alumina is thus obtained.
[0071] The temperature and pressure ranges for hot isostatic pressing are determined so
as to give desirable translucency to the sintered body and improve the mechanical
strength thereof. When the hot isostatic pressing is implemented at the temperature
lower than 1,200°C or under the pressure lower than 1,000 atm, sufficient translucency
is not given to the sintered body. When the temperature is over 1,250°C, on the other
hand, abnormal grain growth lowers both translucency and mechanical strength. When
the pressure is over 2,000 atm, even very small pores or scratches in the sintered
body may cause fatal cracks due to stress concentration.
[0072] Both ends of the multi-pipe emission tube 1M of translucent alumina are then ground
with a diamond grinding wheel, and the inner and outer surface of the emission tube
1M is ground and polished to have the wall thickness not greater than 0.2 mm by using
a brush with diamond abrasive grains (grain diameter: 0.5 micrometer) (process 7).
This grinding process smooths the surface of the emission tube to prevent scattering
of light on the surface, thus improving the linear transmittance.
[0073] Through the process 1 to 7, obtained is the emission tube 1M shown in Fig. 4, consisting
of three single emission pipes 1m1, 1m2, and 1m3, which are integrally formed adjacent
to and parallel to one another and have the common side wall shown by the shaded parts
in the drawing. The emission tube 1M thus prepared has the inner diameter of about
4.0 mm (wall thickness: approximately 0.2 mm) and the total length of approximately
40 mm.
[0074] The emission tube 1M with pairs of primary electrodes is, in use, installed in the
outer bulb of the variable color lamp. Luminescent materials are individually sealed
in each of the single emission pipes 1m1, 1m2, and 1m3 of the emission tube 1M. Examples
of such luminescent materials include: indium halide emitting bluish purple line spectrum,
thallium halide emitting green line spectrum, and sodium halide emitting reddish orange
line spectrum. In one embodiment, indium halide is sealed in the single emission pipe
1m1; thallium halide in the single emission pipe 1m2; and sodium halide in the single
emission pipe 1m3.
[0075] The variable color lamp of the second embodiment has the multi-pipe emission tube
1M consisting of the three single emission pipes 1m1, 1m2, and 1m3 integrally formed
adjacent to and parallel to one another, while the first embodiment has three independent
emission tubes 3 through 5 installed in the outer bulb. The second embodiment has
the following effects as well as those of the first embodiment including variation
of the luminous color corresponding to the color matching functions of the chromaticity
coordinate system.
[0076] In the integral emission tube 1M of the variable color lamp, the side wall of the
adjacent single emission pipes 1m1 and 1m2 or 1m2 and 1m3 is formed in common. Thermal
energy is freely transferred between the adjacent single emission pipes through the
common side wall, thus allowing the wall temperature of the single emission pipes
1m1, 1m2, and 1m3 to rise uniformly. The whole emission tube 1M is accordingly stabilized
within a short time period, and the warm-up time is favorably shortened.
[0077] When plural emission tubes are arranged not in contact with or adjacent to one another
in the lamp, arc discharge between the pair of primary electrodes starts at a different
moment in each emission tube, and heat generation due to arc discharge is made different
among the tubes. The plural emission tubes differ in the heating time period for raising
the wall temperature of the emission tube to a predetermined value (the temperature
at which sealed discharge material is evaporated in the emission tube to give saturated
vapor pressure). Accordingly the plural emission tubes are not stabilized at the same
time or on the whole within a short time.
[0078] On the contrary, in the structure of the multi-pipe emission tube 1M, the temperature
of the single emission pipes increase uniformly to a predetermined value based on
heat transfer through the common wall. The plural emission pipes or the whole emission
tube 1M is thus stabilized almost simultaneously and the warm-up time of the variable
color lamp is significantly shortened.
[0079] Heat transfer between the adjacent single emission pipes 1m1 and 1m2 or 1m2 and 1m3
of the emission tube 1M expands the possible dimmer range of each single emission
pipe.
[0080] A high intensity discharge lamp including an emission tube generally has a dimmer
range of approximately ten percent. The dimmer range of the discharge lamp is significantly
narrower than incandescent lamps and tungsten halogen lamps because of the following
reasons. In the high intensity discharge lamp, when input to the emission tube is
limited in order to decrease the light flux, the temperature in the emission tube
is lowered and the luminescent material such as In, Tl, or Na sealed in the emission
tube varies its partial vapor pressure. When the partial vapor pressure drops down
to a predetermined threshold or lower value, the lamp does not discharge any light
but is in 'OFF' state. In the conventional high intensity discharge lamp with only
one emission tube, the possible dimmer range is within approximately ninety percent
of the rated output. In the variable color lamp 1 of the first embodiment including
independent three emission tubes, the possible dimmer range is also about ninety percent.
[0081] In the emission tube 1M of the second embodiment, on the other hand, since three
single emission pipes are arranged adjacent to and parallel to one another and have
the common side wall, thermal energy generated from each emission pipe is transferred
to the other emission pipes through the side wall. Even when input to one emission
pipe is limited, thermal energy generated from the adjacent emission pipes is given
to that one pipe. Accordingly the single emission pipe with limited input in the emission
tube 1M of the variable color lamp is maintained at higher temperature than the only
one emission tube with limited input in the conventional high intensity discharge
lamp. The partial vapor pressure of the luminescent material sealed in the single
emission pipe with limited input does not vary but is kept relatively constant, so
that the possible dimmer range of the variable color lamp becomes wider.
[0082] Input to one emission pipe may be decreased while input to the other two emission
pipes is increased. This allows the total input to the whole emission tube to be kept
constant and thereby prevents the temperature fall of the single emission pipe with
limited lower input so as to attain a wider dimmer range.
[0083] The variable color lamp with the emission tube 1M has wider variation of chromaticity
of the emitted light corresponding to the wider dimmer range of the emission tube.
[0084] Arrangement of the single emission pipes with metal halides sealed therein attains
the following effects besides the wider dimmer range.
[0085] In the emission tube 1M of the embodiment, the single emission pipe 1m2 disposed
in the middle contains indium halide emitting bluish purple line spectrum and having
a narrower dimmer range than thallium and sodium. Thallium halide emitting green line
spectrum is in the single emission pipe 1m1, and sodium halide emitting reddish orange
line spectrum in the single emission pipe 1m3. When input to the middle emission pipe
1m2 with indium halide having a relatively narrow dimmer range is decreased and the
same to the adjacent emission pipes 1m1 and 1m3 is increased, thermal energy generated
from the adjacent emission pipes 1m1 and 1m3 is transferred to the middle emission
pipe 1m2 so as to maintain the middle emission pipe at high temperature. The possible
dimmer range of the middle emission pipe 1m2 is thus made wider than the original
dimmer range of indium. Another emission tube 1N shown in Fig. 6 may be used for the
emission tube 1M to give the similar effects.
[0086] The properties of the emission tube 1M are given below:
Linear transmittance to visible light (wavelength: 380 to 760 nm): not less than 70%
Linear transmittance to light having the wavelength of 500 nm: 82% (wall thickness:
0.5 mm)
Average grain diameter: approximately 0.7 micrometer
(maximum grain diameter: 1.4 micrometer)
Mechanical strength (JIS R1601)
Bending strength St: (room temperature) = 98 kg/cm²
(900°C) = 81 kg/cm²
Weibull coefficient: (room temperature) = 9.3
(900°C) = 8.1
Above data including the grain diameter and the mechanical strength was determined
not for the emission tube 1M itself of the embodiment but for a sample prepared under
the various conditions specified in the above manufacturing process (the shape and
the thickness of the sample were in conformity with JIS R1601).
[0087] The grain diameter was determined in the following manner. The surface of the sample
prepared to have the shape and thickness in accordance with JIS R1601 was lapped with
diamond abrasive grains and exposed to molten potassium hydroxide for intergranular
etching. The image of the grain was analyzed based on observation of the surface of
the sample with a scanning electron microscope. For the image analysis, the grain
was assumed to be spherical or polygonal, and the maximum value of the diameter or
the distance between vertexes was used for calculation of the grain diameter. Fig.
7 shows a distribution diagram of the grain diameter determined by assuming the spherical
grain.
[0088] The sample was cut to have the thickness of 0.5 mm and finished by lapping the surface,
and the linear transmittance was measured with a double beam spectrophotometer.
[0089] Observation of the tissue with a transmission electron microscope (TEM) did not show
any grain boundary phase, undesirable pore in the grain, nor lattice defect, which
may cause scattering of light.
[0090] The emission tube 1M is composed not of the conventional translucent alumina, which
is sintered with a sintering accelerator such as MgO to make large rough grains, but
of fine powdery alumina. The excellent translucency of the alumina of the embodiment
may be ascribed to the following reasons.
[0091] Since alumina (before sintering) contains only a very little amount of impurity (maximum:
0.01 mol%), all the impurity is molten in the alumina and does not substantially form
any grain boundary phase such as a spinel phase. Effects of the grain boundary phase,
which causes scattering of light, are thus eliminated, and the linear transmittance
to the visible light is sufficiently improved.
[0092] Another possible reason is further given below.
[0093] When both the cross sections of the grain and the grain element are assumed to be
circular, the following equation (1) is held. Here, the grain of the diameter D consists
of n grain elements of the diameter d.
[0094] The value of n determined by the equation (1) represents the number of the interface
between grain elements contained in the cross section of a grain.
[0095] The lattice constant was determined with an X-ray diffractometer for various translucent
alumina grains (average grain diameter: 0.72, 0.85, 0.99, 1.16, 1.35, and 1.52 micrometer)
of highly pure alumina. The diameter d of the translucent alumina grain element was
then determined for the various translucent alumina grains above by substituting the
value of the (012) diffraction peak in Scherrer's expression which defines the relationship
between the diameter d of the grain element and the width of the diffraction line.
The results show that the diameter d of the grain element is constant irrespective
of the size of the grain. The Scherrer's expression is shown in 'P. Gallezot, Catalysis,
Science, and Technology; vol. 5; p221, Springer-Verlag (1984)' or 'P. Scherrer; Gottinger
Nachrichen; 2; 98, (1918)'.
[0096] The above equation (1) accordingly proves that the smaller average diameter D of
the grain implies the smaller number of the interface between grain elements in one
grain.
[0097] When light enters polycrystal such as ceramics, it is scattered on the face with
the discontinuous refractive index or discontinuous atomic arrangement. The interface
between the grain elements in the grain has discontinuous atomic arrangement and thus
causes scattering of light. The smaller number of the interface between the grain
elements in the grain, that is, the smaller diameter D of the grain eliminates undesirable
effects of the interface, which cause scattering of light, and improves the linear
transmittance to the visible light.
[0098] Some modification of the above embodiment is described hereinafter.
[0099] The three emission pipes are arranged in parallel on the same plane in the second
embodiment. Three single emission pipes may, however, be disposed in contact with
and parallel to one another to have the common side wall as shown in Fig. 8. In this
structure, an emission tube 1L consists of the three emission pipes integrally formed
with the excessive wall around the pipes. Indium halide, thallium halide, and sodium
halide are separately sealed in the emission pipes of the emission tube 1L in the
same manner as the second embodiment.
[0100] A variable color lamp with the emission tube 1L has the following effects as well
as expansion of the possible dimmer range and the shortened warm-up time described
in the second embodiment. The circumference of the emission tube 1L does not have
any convex or concave but is smooth, and the cross section of the whole emission tube
is a round triangle. The smooth surface efficiently prevents concentration of the
thermal stress generated on sintering or switching, which may cause early rupture
of the lamp, and the life of the variable color lamp is elongated.
[0101] Although each emission pipe of the emission tube is linearly formed in the second
embodiment and the above modification, a U-shaped emission pipe may be used instead.
An emission tube 1R or 1S which consists of three U-shaped emission pipes integrally
formed adjacent to and parallel to one another as shown in Figs. 9 and 10 may, for
example, be installed in the outer bulb of the lamp.
[0102] A variable color lamp with the emission tube 1R or 1S has the following effects as
well as expansion of the possible dimmer range and the shortened warm-up time described
in the second embodiment. The center of emission having the maximum luminous flux
is located on a curved portion in the emission tube 1R or 1S. When such an emission
tube is installed in the outer bulb, the emission center faces the end of the lamp.
The variable color lamp can thus be formed relatively small and space-saving in the
direction of emission.
[0103] Manufacture of the emission tube 1R or 1S is briefly described. The emission tube
1R is prepared with a combination mold shown in Fig. 9, which includes an upper mold
50, a lower mold 51, and a sliding mold 52 slidably disposed between the upper and
the lower molds 50 and 51. Each mold has three arc-shaped grooves to form the cavity
corresponding to the outer face of the emission tube 1R. Another combination mold
with rectangular grooves is used for manufacturing the emission tube 1S having the
polygonal or rectangular cross section.
[0104] The emission tube 1S or 1R is prepared with such a mold according to the following
process. Here manufacture of a single U-shaped emission tube 1A shown in Figs. 11(a)
and 11(b) is described based on the process chart of Fig. 12 for clarity and simplicity
of the description. Fig. 11(b) is a Y-plane cross sectional view of Fig. 11(a).
[0105] High purity (at least 99.99 mol%) of fine powdery alumina (secondary aggregate) prepared
by spray drying in the same manner as the second embodiment is mixed with an organic
binder such as acrylic emulsion, a deflocculant such as sodium polyacrylate, an antifoamer
such as octanol, and distilled water. The mixture is wet stirred with a plastic or
nylon ball mill for approximately twenty four hours, so that excessive aggregation
of alumina is eliminated and alumina uniformly dispersed in the solvent, that is,
slurry, is prepared (process 1).
[0106] The contents of the additives with respect to 100 g of fine powdery alumina are as
follows:
Organic binder: 3g
Deflocculant: 1g
Antifoamer: 0.1g
Distilled water : 55g
Blow holes are then removed from the slurry (process 2). Slurry taken out of the
ball mill is placed in a resin vessel in a vacuum desiccator and stirred with a magnetic
stirrer while air in the desiccator is aspirated with a vacuum pump for several minutes
(for example, five minutes).
[0107] The molded body 1A shown in Figs. 11(a) and 11(b) is prepared with a combination
mold 60 shown in Fig. 13(a) through the following process. As described above, the
emission tube 1R, which is actually applied to the embodiment, is formed with the
combination mold consisting of the upper mold 50, the lower mold 51, and the sliding
mold 52.
[0108] The combination mold 60 includes symmetrical molds 61a and 61b, which are composed
of a porous inorganic material such as plaster or a porous resin containing pores
having the similar function to plaster, as shown in Fig. 13(a). A cavity 63 for slurry
pour is formed between the joint faces of the molds 61a and 61b.
[0109] Each mold 61a or 61b has a U-shaped groove or cavity 63a or 63b on a joint face 65a
or 65b thereof as seen in Fig. 13(b). The groove 63a or 63b has a ridge 64a or 64b
on the center thereof, which is a little lower than the joint face 65a or 65b. The
grooves may previously be molded or cut by using an end mill with spherical teeth
on the edge (not shown).
[0110] After removal of blow holes from the slurry at process 2, the slurry is poured into
the cavity 63 of the combination mold 60 and stood for a predetermined time period
(process 3). An excessive amount (more than the volume of the cavity 63) of slurry
is poured into a cylindrical body 67 mounted on the upper face of the combination
mold 60 as shown in Fig. 14. The lower face of the cylindrical body 67 and the upper
face of the combination mold 60 are sealed with clay or rubber 69.
[0111] The solvent (distilled water in the embodiment) contained in the slurry, which is
poured into the cavity 63, is absorbed into the pores of the porous molds 61a and
61b while the slurry is stood for the predetermined time period. Alumina grains bound
to one another via the organic binder are uniformly aligned along the wall of the
cavity 63, and an alumina layer SA is formed as shown in Fig. 15.
[0112] The thickness of the alumina layer SA or the inner diameter of the molded body depends
on the standing time period. The standing time is thus previously determined through
experiments such that the alumina layer SA formed has a desirable inner diameter.
The standing time and the dimensions of the groove should be determined by considering
the volume shrinkage on sintering. In one embodiment, the standing time is three minutes
or shorter to make the inner diameter of the alumina layer SA around 4.82 mm, and
the packing ratio approximately 58%. The outer diameter of the alumina layer SA is
determined by the dimensions of the cavity 63, and is around 5.54 mm in the embodiment.
[0113] The mold may be stood under the negative pressure so that the solvent in the slurry
is forcibly aspirated out of the mold. This system attains shorter standing time,
direct removal of blow holes from the slurry, and higher packing ratio.
[0114] After elapse of the predetermined standing time, slurry remaining in the cylindrical
body 67 or on the inner face of the alumina layer SA is removed (process 4). The combination
mold 60 is separated into two parts, and the molded body 1A shown in Figs. 11(a) and
11(b) is parted from the mold. The molded body is dried until the solvent is completely
eliminated therefrom (process 5).
[0115] The molded body is sintered through heat treatment at a predetermined sintering temperature
between 1,200 and 1,300°C, for example, at 1,235°C for four hours (process 6). Here
the heating rate is 100°C / hour. Through the sintering process, the volume of the
molded body is shrunk to approximately 83%, and the packing factor of the sintered
body becomes approximately 100% (bulk density: 3.976).
[0116] The sintering temperature is set in the range of 1,200 to 1,300°C so as to make the
actual density of the sintered body not less than 95% of the theoretical density for
the following hot isostatic pressing and prevent growth of undesirable rough crystals.
When the temperature is 1,200°C or lower, the density of the sintered body drops to
the level unsuitable for hot isostatic pressing, that is, less than 95% of the theoretical
density. When the temperature is, on the other hand, over 1,300°C, formation of rough
crystals decreases the strength of the sintered body.
[0117] The sintered body is exposed to hot isostatic pressing in argon atmosphere or the
atmosphere of argon with oxygen of not greater than 20vol% (process 7). The conditions
of the hot isostatic pressing are given below; here the heating rate is 200°C / hour:
Temperature: 1,200 to 1,250°C
(optimum temperature: 1,230°C)
Pressure: 1,000 to 2,000 atm
(optimum pressure: 1,000 atm)
Time: one to four hours (optimum time: two hours)
The sintered body acquires translucency through this process, and the emission tube
1A of translucent alumina is thus obtained. The sintered body is embedded in sapphire
beads (diameter: 2 mm) or titanium sponge during the hot isostatic pressing.
[0118] The temperature and pressure ranges for hot isostatic pressing are determined so
as to give desirable translucency to the sintered body and improve the mechanical
strength thereof. When the hot isostatic pressing is implemented at the temperature
lower than 1,200°C or under the pressure lower than 1,000 atm, sufficient translucency
is not given to the sintered body. When the temperature is over 1,250°C, on the other
hand, abnormal grain growth lowers both translucency and mechanical strength. When
the pressure is over 2,000 atm, even very small pores or scratches in the sintered
body may cause fatal cracks due to stress concentration.
[0119] The emission tube 1A thus prepared has the inner diameter of about 4.0 mm, the wall
thickness of approximately 0.3 mm, and the length between the opening and the curve
of approximately 20 mm, that is, the total length of approximately 40 mm. Observation
of the tissue with a transmission electron microscope (TEM) did not show any grain
boundary phase, undesirable pore in the grain, nor lattice defect, which may cause
scattering of light.
[0120] The inner and outer surface of the emission tube 1A is ground and polished to have
the wall thickness not greater than 0.2 mm by using a brush with diamond abrasive
grains (grain diameter: 0.5 micrometer) (process 8). This grinding process smooths
the surface of the emission tube to prevent scattering of light on the surface, thus
improving the linear transmittance. The wall of the tube may be ground to the thickness
of 0.05 mm according to the requirements.
[0121] The emission tube 1A thus prepared, that is, the emission tube 1R or 1S, has almost
the same linear transmittance and average grain diameter as the emission tube 1M of
the second embodiment, and possesses the mechanical strength of approximately 80%
of the emission tube 1M.
Industrial Applicability
[0122] The variable color lamp of the invention described above may be applied to neon signs
as well as lighting in or out of the houses or illumination at shop windows.