Electric lamp or space discharge component or device manufacturi – Process – With assembly or disassembly
Reexamination Certificate
2001-06-25
2004-01-20
O'Shea, Sandra (Department: 2875)
Electric lamp or space discharge component or device manufacturi
Process
With assembly or disassembly
C313S574000
Reexamination Certificate
active
06679746
ABSTRACT:
BACKGROUND OF THE INVENTION
The present invention relates to a discharge lamp and a lamp unit. In particular, the present invention relates to a discharge lamp and a lamp unit used as the light source of an image projection apparatus such as a liquid crystal projector or a digital micromirror device (DMD) projector.
In recent years, an image projection apparatus such as a liquid crystal projector or a projector using a DMD has been widely used as a system for realizing large-scale screen images. A high-pressure discharge lamp having a high intensity has been commonly and widely used in such an image projection apparatus. For the light source used in the image projection apparatus, light is required to be concentrated on an imaging device included in the optical system of the projector, so that in addition to high intensity, it is also necessary to achieve a light source close to a point light source. Therefore, a short arc ultra high pressure mercury lamp that is closer to a point light and has a high intensity has been noted widely as a promising light source.
Referring to 
FIG. 4
, a conventional short arc ultra high pressure mercury lamp 
1000
 will be described. 
FIG. 4
 is a schematic view of an ultra high pressure mercury lamp 
1000
. The lamp 
1000
 includes a substantially spherical luminous bulb 
110
 made of quartz glass, and a pair of sealing portions (seal portions) 
120
 and 
120
′ also made of quartz glass and connected to the luminous bulb 
110
.
A discharge space 
115
 is inside the luminous bulb 
110
. A mercury (in an amount of, for example, 150 to 250 mg/cm
3
) as a luminous material, a rare gas (e.g., argon with several tens kPa) and a small amount of halogen are enclosed in the discharge space 
115
. A pair of tungsten electrodes (W electrode) 
112
 and 
112
′ are opposed with a certain electrode distance D (e.g., about 1.5 mm) in the discharge space 
115
. Each of the W electrodes 
112
 and 
112
′ includes an electrode axis (W rod) 
116
 and a coil 
114
 wound around the head of the electrode axis 
116
. The coil 
114
 has a function to reduce the temperature at the head of the electrode.
The electrode axis 
116
 of the W electrode 
112
 is welded to a molybdenum foil (Mo foil) 
124
 in the sealing portion 
120
, and the W electrode 
112
 and the Mo foil 
124
 are electrically connected by a welded portion where the electrode axis 
116
 and the Mo foil 
124
 are welded. The sealing portion 
120
 includes a glass portion 
122
 extending from the luminous bulb 
110
 and the Mo foil 
124
. The glass portion 
122
 and the Mo foil 
124
 are attached tightly so that the airtightness in the discharge space 
115
 in the luminous bulb 
110
 is maintained. In other words, the sealing portion 
120
 is sealed by attaching the Mo foil 
124
 and the glass portion 
122
 tightly for foil-sealing. The sealing portions 
120
 have a substantially circular cross section, and the rectangular Mo foil 
124
 is disposed in the center of the inside of the sealing portion 
120
.
The Mo foil 
124
 of the sealing portion 
120
 includes an external lead (Mo rod) 
130
 made of molybdenum on the side opposite to the side on which the welded portion is positioned. The Mo foil 
124
 and the external lead 
130
 are welded to each other so that the Mo foil 
124
 and the external lead 
130
 are electrically connected at a welded portion 
132
. The configurations of the W electrode 
112
′ and sealing portion 
120
′ are the same as those of the W electrode 
112
 and sealing 
120
, so that description thereof will be omitted.
Next, the operational principle of the lamp 
1000
 will be described. When a start-up voltage is applied to the W electrodes 
112
 and 
112
′ via the external leads 
130
 and the Mo foils 
124
, discharge of argon (Ar) occurs. Then, this discharge raises the temperature in the discharge space 
115
 of the luminous bulb 
110
, and thus the mercury is heated and evaporated. Thereafter, mercury atoms are excited and become luminous in the arc center between the W electrodes 
112
 and 
112
′. The higher the mercury vapor pressure of the lamp 
1000
 is, the higher the emission efficiency is, so that a lamp having a higher mercury vapor pressure is more suitable as a light source for an image projection apparatus. However, in view of the physical strength against pressure of the luminous bulb 
110
, the lamp 
1000
 is used at a mercury vapor pressure of 15 to 25 MPa.
The conventional lamp 
1000
 is produced in the manner as shown in 
FIGS. 5A
 to 
5
C. 
FIGS. 5A
 to 
5
C are cross-sectional views showing a production process sequence of a method for producing the lamp 
1000
.
First, a glass pipe 
150
 for a discharge lamp having a luminous bulb portion 
110
 that will be formed into the luminous bulb of the lamp 
1000
 and a side tube portion (sealing portion) 
122
 that will be formed into the sealing portion of the lamp 
1000
, and an electrode assembly 
140
 in which the electrode 
112
 is joined to one end of the metal foil (Mo foil) 
124
 and the external lead 
130
 is joined to the other end are prepared. Then, as shown in 
FIG. 5A
, the electrode assembly 
140
 is inserted in the glass pipe 
150
 for a discharge lamp (electrode assembly insertion process).
Next, as shown in 
FIG. 5B
, when the pressure in the glass pipe 
150
 is reduced (e.g., less than 1 atmospheric pressure), and the glass tube 
122
 of the glass pipe 
150
 is heated and softened with, for example, a burner 
54
, so that the side tube portion 
122
 and the Mo foil 
124
 are attached tightly, thereby forming the sealing portion 
120
 (sealing portion formation process).
The same processes as those shown in 
FIGS. 5A and 5B
 are performed to the other side tube portion. More specifically, another electrode assembly 
140
 is inserted into a side tube portion that has not been formed into a sealing portion yet. At this time, the electrode assembly 
140
 is inserted while being aligned with the electrode 
112
 of the already-sealed electrode assembly 
140
 in such a manner that the pair of electrodes are on the same axis as much as possible and a predetermined electrode distance D is achieved. Thereafter, the sealing portion formation process is performed.
In this manner, when the sequence of the electrode assembly insertion process and the sealing portion formation process is performed twice, the luminous bulb 
110
 in which the pair of electrodes 
112
 are arranged in the discharge space 
115
 sealed with the pair of sealing portions 
120
 can be formed, as shown in FIG. 
5
C. Thus, the lamp 
1000
 can be produced. The luminous material enclosed in the discharge space 
115
 can be introduced into the luminous bulb 
110
 after one sealing portion 
120
 is formed and before the other sealing portion 
120
 is formed.
The electrode distance D of the lamp 
1000
 is a very important design matter that defines the arc length of the discharge lamp. When the electrode distance D of the lamp 
1000
 is short, a discharge lamp serving as a light source closer to a point light source and having higher intensity can be realized. However, the inventors of the present invention found that there are limitations of the conventional production method regarding further reduction of the electrode distance D. More specifically, the inventors of the present invention found limitations in the production process as follows. In the conventional production method, it is necessary to define the electrode distance D in the electrode assembly insertion process shown in 
FIG. 5A
, so that the electrode distance D cannot be defined with a higher precision than that of the alignment in the electrode assembly insertion process.
Since the electrode assembly 
140
 has a configuration where the W rod 
116
 and the external lead 
130
 are joined to ends of a thin Mo foil 
124
 (e.g., a thickness of about 20 to 30 &mgr;m), it is difficult to improve the alignment precision because of the small thickness of the Mo foil 
124
. Therefore, when the lamp 
1000
 is produced by the conventional production me
Horiuchi Makoto
Ichibakase Tsuyoshi
Kai Makoto
Sasaki Ken-ichi
Seki Tomoyuki
Harness & Dickey & Pierce P.L.C.
Macchiarolo Peter
Matsushita Electric - Industrial Co., Ltd.
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