Patent Grant
7038379
1. Field of the Invention
The present invention relates to a high pressure discharge lamp and a method for sealing a bulb of the high pressure discharge lamp. More specifically, the present invention relates to a high pressure discharge lamp which may be used as a light source for such devices as a copier or a projector and which, even after being lit for a considerably long time, does not have problems such as a blowout of the bulb made of quartz glass or the blackening of the quartz glass bulb, and a method for sealing a bulb used in such a high pressure discharge lamp.
2. Description of the Related Art
In general, high pressure discharge bulbs have a structure in which each electrode of a pair of electrodes (i.e., an anode and a cathode) is disposed so as to be opposite the other in a quartz glass bulb, which includes an expanded portion for luminescence and a sealing portion, and the anode and the cathode are joined by, for instance, welding with molybdenum foil. Also, the sealing portion of the quartz glass bulb is airtightly sealed by, for example, welding with molybdenum foil. A gas for assisting an electric discharge, such as mercury vapor, is contained in the expanded portion for luminescence of the quartz glass bulb which has been airtightly sealed.
In general, high pressure discharge lamps which may be represented by a xenon lamp, a high pressure mercury lamp, and a metal halide lamp, have high brightness and excellent color rendering properties, and are used as light sources for such devices as a copier or a projector.
In the above-mentioned high pressure discharge lamp, an external lead wire (not shown in the figure) is connected to the Mo foils 3a and 3b, which are sealed at their respective ends of the quartz glass bulb 1, and a predetermined trigger voltage is applied to the external lead wires. When the trigger voltage is applied, a glow discharge is induced between the electrodes 2a and 2b in the inert gas atmosphere thereby vaporizing mercury contained in the quartz glass bulb 1, and this causes a plasma discharge in the high pressure mercury vapor. The light emitted by the plasma discharge has high brightness and excellent color rendering properties.
As mentioned above, in the high pressure discharge lamp, an inert gas is contained and sealed in the quartz glass bulb 1 as a starting gas for the glow discharge, and the charged pressure thereof is between 6 kPa and 60 kPa (preferably between 20 kPa and 50 kPa). For this reason, the difference in pressure between the inside and outside of the quartz glass bulb 1, i.e., the difference between the atmospheric pressure and the charged pressure, is in the range between 41 kPa and 95 kPa. As a method for carrying out airtight-sealing of the quartz glass bulb 1, a pinch sealing method and a shrink sealing method are known.
The pinch sealing method is a method in which an outer periphery portion of a quartz glass bulb is collapsed and sealed by pressure applied using a force piston provided with a metallic mold. This method is mainly used for a sealing process in which the internal pressure of an object is about 4–5 MPa. If the pinch sealing method is employed, however, residual distortion tends to be generated after applying pressure. Also, stress concentrations tend to be caused since the shape of the quartz glass bulb and that of a sealing metal at the contacting portion thereof are significantly different. Accordingly, if the pinch sealing method is applied to the above-mentioned high pressure discharge lamp, there is a danger that the quartz glass bulb 1 may blow out.
The shrink sealing method, on the other hand, is a method in which an outer periphery of both ends of a quartz glass bulb is heated while the pressure difference between the inside and outside of the quartz glass is maintained, and, thereafter, the quartz glass bulb is naturally shrunk in order to airtightly seal the bulb. The shrink sealing method is applicable to a sealing process in which the internal pressure of a quartz glass bulb is 20 MPa or greater. According to this method, contrary to the pinch sealing method, a forced pressure is not applied to the bulb and residual distortion does not tend to be generated since the quartz glass bulb is subjected to natural shrinkage. Also, since the shape of the quartz glass bulb and that of a sealing metal foil are substantially the same, stress concentration tends not to be caused. For this reason, the shrink sealing method is often used as the sealing process for the above-mentioned high pressure discharge lamp.
However, in the conventional shrink sealing method, the difference between the thermal expansion coefficient of the quartz glass bulb and that of the electrodes is not considered at all when carrying out the sealing process of the bulb of a high pressure discharge lamp. Also, a heating step for the quartz glass bulb during the sealing process is conventionally carried out manually and it was difficult to obtain an accurate target length of a contacting portion which is formed by contacting an electrode with the quartz glass bulb at the sealing portion. For the case where the length of the contacting portion formed by the electrode and the quartz glass bulb at the contacting portion is relatively long, cracks may be generated at the sealing portions, as shown in
On the other hand, when a conventional high pressure discharge lamp is used, sputtering is vigorously caused and this causes blackening of the quartz glass bulb in a relatively short amount of time. Also, if the amount of halogen gas contained in the high pressure discharge lamp is increased to enhance the halogen cycle efficiency in order to prevent the blackening caused by the electrode sputtering, the sealing portion of the electrode tends to be eroded by the halogen gas and this eventually causes a blowout of the quartz glass bulb.
Accordingly, an object of the present invention is to solve the above-mentioned problems and provide a high pressure discharge lamp and a method for sealing a bulb thereof by which the generation of cracks during the sealing process may be suppressed and problems such as the falling of an electrode are not caused.
Another object of the present invention is to provide a high pressure discharge lamp by which a blowout of the quartz glass bulb or the blackening of the quartz glass bulb may be prevented even after being lit for a considerably long time.
The inventors of the present invention, after pursuing diligent studies to achieve the above-mentioned objectives, have noticed the importance of the length L of the contacting portion which is formed by contacting the electrode and the quartz glass bulb at the sealing portion be in the range between Lmax (mm)≦200/(P×D) (the maximum length) and Lmin (mm)≧0.8/(D2×π) or Lmin (mm)≧0.7 whichever is longer (the minimum length), where D is the diameter (mm) of the electrode and P is the power (W) supplied to the high pressure discharge lamp.
Also, the inventors of the present invention have noticed the importance in the roughness of the surface of an end portion of the electrode and discovered that if the maximum value (hereinafter referred to as “Rmax”) of the surface roughness (hereinafter referred to as “R”) of the end portion of the electrode is less than a certain value, it becomes possible to significantly decrease the sputtering of the electrode and, hence, prevent the blackening of the quartz glass bulb. The inventors of the present invention have also discovered that if the Rmax value of portions of the electrode other than the end portion is within in a certain range, it becomes possible to prevent a blowout of the quartz glass bulb.
The present invention provides a high pressure discharge lamp including: a quartz glass bulb; a conductive element which is airtightly sealed at a sealing portion of the quartz glass bulb; and a pair of electrodes, each electrode of the pair of electrodes being disposed in the quartz glass bulb so as to be opposite the other and each electrode of the pair of electrodes being connected to the conductive element, wherein a part of each electrode of the pair of electrodes is sealed with the quartz glass bulb at the sealing portion so as to generate a contacting portion formed by the part of each electrode of the pair of electrodes and the quartz glass bulb, and the maximum length, Lmax, of the contacting portion is defined as:
Lmax(mm)≦200/(P×D); and
In accordance with one aspect of the invention, the conductive element is molybdenum.
In accordance with another aspect of the invention, the maximum value, Rmax, of the surface roughness of the pair of electrodes at the contacting portion is about 5 μm or less, where Rmax is the maximum of the absolute value of the difference between the distance from the axial center of each of the electrodes to a particular point on the surface of each of the electrodes and the mean value of the distance.
In yet another aspect of the invention, the maximum value, Rmax, of the surface roughness of the pair of electrodes at the contacting portion is in the range between about2 μm and 3 μm.
The present invention also provides a method for sealing a bulb of a high pressure discharge lamp including a first electrode and a second electrode, the first and second electrodes being disposed in the bulb having a first insertion opening and a second insertion opening so as to be opposite the other, comprising the steps of: disposing the first electrode at the first insertion opening so that the first electrode is placed at a predetermined position in the axial direction of the electrode; heating a predetermined portion of the first insertion opening while maintaining a pressure difference between the inside and outside of the bulb; shrinking the predetermined portion of the first insertion opening in a natural state so that a part of the first electrode is sealed with the predetermined portion; disposing the second electrode at the second insertion opening so that the second electrode is placed at a predetermined position in the axial direction of the electrode; heating a predetermined portion of the second insertion opening while maintaining a pressure difference between the inside and outside of the bulb; and shrinking the predetermined portion of the second insertion opening in a natural state so that a part of the second electrode is sealed with the predetermined portion, wherein the length of a contacting portion formed by sealing the part of the first electrode with the bulb, and by the part of the second electrode with the bulb, is in the range between:
The present invention also provides a high pressure discharge lamp including: a quartz glass bulb; conductive elements, the conductive elements being airtightly sealed at sealing portions of the quartz glass bulb; and a pair of electrodes, each electrode of the pair of electrodes being disposed so as to be opposite the other and each electrode being connected to one of the conductive elements, wherein Rmax of an end portion of each of the electrodes is about 5 μm or less. Note that in this specification, the term “Rmax” means the maximum of the absolute value of the difference between the distance from the axial center of an electrode to a particular point on the surface of the electrode and the mean value of the distance.
In accordance with one aspect of the invention, the conductive element is molybdenum.
In accordance with another aspect of the invention, the length of the end portion of each electrode is in the range between about P/150 and P/100 mm from an end of each electrode along the length of each electrode, where P is a supplied power to the high pressure discharge lamp in watts.
In yet another aspect of the invention, the maximum value of the surface roughness of the end portion of each of the electrodes is about 3 μm or less.
In yet another aspect of the invention, the maximum value of the surface roughness of the end portion of each of the electrodes is about 1 μm or less.
In yet another aspect of the invention, the maximum value of the surface roughness of the end portion of each of the electrodes is about 0.5 μm or less.
In yet another aspect of the invention, the maximum value of the surface roughness of a portion other than the end portion of each of the electrodes is in the range between about 5 μm and 12 μm.
In yet another aspect of the invention, the maximum value of the surface roughness of a portion other than the end portion of each of the electrodes is in the range between about 7 μmm and 9 μm.
In yet another aspect of the invention, mercury vapor is contained in the high pressure discharge lamp in an amount between about 0.12 and 0.3 mg/mm3.
In yet another aspect of the invention, a halogen gas is contained in the high pressure discharge lamp in an amount between about 10−8 and 10−2 μmol/mm3.
In yet another aspect of the invention, an inert gas is contained in the high pressure discharge lamp with a pressure of about 6 kPa or more.
In yet another aspect of the invention, the pair of electrodes uses tungsten containing potassium oxide.
In yet another aspect of the invention, the bulb wall loading in the high pressure discharge lamp is about 0.8 W/mm2 or more.
In yet another aspect of the invention, the end portion of each of the electrodes has a surface which is polished by a composite electrolytic polishing method.
Some of the features and advantages of the invention have been described, and others will become apparent from the detailed description which follows and from the accompanying drawings, in which:
The invention summarized above and defined by the enumerated claims may be better understood by referring to the following detailed description, which should be read with reference to the accompanying drawings. This detailed description of a particular preferred embodiment, set out below to enable one to build and use one particular implementation of the invention, is not intended to limit the enumerated claims, but to serve as a particular example thereof.
In the high pressure discharge lamp according to this embodiment of the invention, as shown in
The length L of the contacting portion which is formed by contacting the electrode 2a and the quartz glass bulb 1 at the sealing portion is defined as follows:
The same definition is also applied to the length of the contacting portion formed by contacting the electrode 2b and the quartz glass bulb 1.
In the high pressure discharge lamp having the length L of the contacting portion formed by the quartz glass bulb 1 and the electrodes 2a and 2b, respectively, since the strength of the contacting portions is not decreased and the generation of cracks at the contacting portions may also be suppressed, the quartz glass bulb 1 will not be blown out even if the lamp is operated with an internal pressure of about 8 MPa or greater.
Next, the basis for the derivation of the above-mentioned condition will be explained in more detail. In the following explanation, a quartz glass bulb 1 containing 0.12–0.30 mg/mm3 of mercury and 10−8−10−2 μmol/mm3 of an inert gas is used as a sample to derive the condition.
Since a defect percentage of less than 1% at the termination of the lifetime of the high pressure discharge lamp is generally required, the maximum length Lmax and the minimum length Lmin of the length L of the contacting portion formed by the electrode and the quartz glass bulb were studied based on the data shown in
If the length L of the contacting portion formed by contacting the electrode and the quartz glass bulb is too long, cracks may be generated during the sealing process for the quartz glass bulb due to the difference between the thermal expansion coefficient of the electrode and the quartz glass bulb.
Accordingly, it is necessary to determine the maximum length of the length L of the contacting portion formed by the electrode and the quartz glass bulb in order to suppress the defect percentage due to the generation of cracks. Based on the data shown in
Lmax(mm)≦200/(P×D)
where D is the diameter (mm) of the electrode and P is the power (W) supplied to the high pressure discharge lamp.
On the other hand, if the length L of the contacting portion formed by contacting the electrode and the quartz glass bulb is too short, the strength of the portion supporting the electrode is weakened and problems such as the falling of the electrode are caused. In order to prevent such problems, it is necessary to determine the minimum length of the length L of a contacting portion formed by the electrode and the quartz glass bulb. The minimum length of the length L of the contacting portion formed by the electrode and the quartz glass bulb depends on the diameter of the electrode and is inversely proportional to an increase in the cross-sectional area of the electrode. The coefficient for the relationship is calculated to be 0.8 based on the data shown in
Lmin(mm)≧0.8/(D2×π)
Note that at least 0.7 mm of contacting portion is known to be required for the construction of a quartz glass bulb and if the contacting portion has a length shorter than 0.7 mm, the defect percentage is significantly increased. Accordingly, the minimum length of the length L of the contacting portion formed by the electrode and the quartz glass bulb needs to satisfy the following condition as well as the above-mentioned condition:
Lmin(mm)≧0.7
Note that a DC power supply may be employed instead of the AC power supply. However, in such a case, the shape of the electrode tip will be different from the one shown in the figure. In general, the electrode for a DC power supply has a sharper tip and the diameter of the cathode is different from that of the anode.
When the high pressure discharge lamp is lighted, a trigger voltage is applied via the external lead wires 4a and 4b to induce a glow discharge between the electrodes 2a and 2b. In this manner, mercury contained in the quartz glass bulb 1 is vaporized and a plasma discharge may be generated in the high pressure mercury vapor so that light having high brightness and excellent color rendering properties may be emitted. When a stable state of the high pressure discharge lamp emitting light is obtained, a control unit (not shown in the figure) controls the electric power so that the power supplied to the high pressure discharge lamp becomes constant. In general, a voltage of about 50–100 V, by the DC or AC power supply, is applied to the external lead wires 4a and 4b in the stable state, and power of about 120–200 W is supplied to the high pressure discharge lamp.
Next, a method for sealing the bulb of a high pressure discharge lamp according to an embodiment of the present invention will be described in more detail.
The high pressure discharge lamp according to an embodiment of the present invention includes a quartz glass bulb having a pair of insertion openings (i.e., a first and a second insertion opening) used for inserting a respective electrode, each of which is disposed at an opposing position relative to the other. The method for sealing the bulb of a high pressure discharge lamp according to an embodiment of the present invention is a two-step method in which one of the pair of electrodes (or a first electrode) is sealed in the first step, and the other one of the pair of electrodes (or a second electrode) is sealed in the second step.
In the first step, the first electrode is disposed at the first insertion opening so that the first electrode is placed at a predetermined position in the axial direction, and the quartz glass bulb is evacuated until the partial pressure of oxygen (O) in the bulb is reduced to 2.5×10−3 Pa or less. At that time, an inert gas may be introduced into the quartz glass bulb so that the pressure of the inert gas contained in the quartz glass bulb becomes about 6 kPa–60 kPa. After the evacuation, the quartz glass bulb is in a vacuum state in which the partial pressure of oxygen (O) in the bulb is 2.5×10−3 Pa or less, or an inert gas with a sealing pressure of about 6 kPa–60 kPa is contained in the bulb. The difference in pressure between the inside and outside of the quartz glass bulb is 101 kPa in the vacuum state and 41 kPa–95 kPa for the case when the inert gas is introduced. While maintaining the pressure difference, an outer periphery of the quartz glass bulb, at which the Mo foil is inserted, is heated and then naturally shrunk so that the Mo foil and a part of the electrode is airtightly sealed with the quartz glass bulb.
In the second step, mercury is introduced into the quartz glass bulb through the second insertion opening, the second electrode is disposed at the second insertion opening so that the second electrode is placed at a predetermined position in the axial direction, and the quartz glass bulb is evacuated until the partial pressure of oxygen (O) in the bulb is reduced to 2.5×10−3 Pa or less. After that, a halogen gas and optionally an inert gas are introduced into the quartz glass bulb. After evacuation, the pressure of the halogen gas and the inert gas contained in the quartz glass bulb is about 6 kPa–60 kPa, and the pressure difference between the inside and outside of the bulb, i.e., the difference between the atmospheric pressure and the charged pressure, is in the range between about 41 kPa and 95 kPa. While maintaining the pressure difference, an outer periphery of the quartz glass bulb, at which the Mo foil is inserted, is heated as in the first step and then the bulb is naturally shrunk so that the Mo foil and a part of the second electrode is airtightly sealed with the quartz glass bulb.
The contact of a quartz glass bulb with an electrode in the sealing process is a physical one, and the melted quartz glass bulb makes contact with the electrode so as to follow the convex-concave surface (rough surface) of the electrode during the sealing process. The quartz glass bulb is then solidified. After the sealing process, when the temperature of the contacting portion is cooled down to an ordinary temperature, the shape of the quartz glass bulb at the contacting portion is subtly different from the shape of the surface of the electrode due to the difference in the thermal expansion coefficient between the two. Accordingly, stress is generated at the sealing portion, and this is also one of the causes of cracks.
As shown in
The maximum value, Rmax, of the surface roughness of an electrode which may be obtained by subjecting a surface to machining is generally about 12 μm. In this embodiment of the present invention, the maximum value, Rmax, of the surface roughness of an electrode at the contacting portion in the range between about 2 μm and 3 μm is realized by carrying out a polishing process after the machining process, such as electrolytic polishing, barrel polishing, or a combination thereof. Electrolytic polishing is a method in which a surface of an electrode is smoothed by immersing the electrode in an acidic solution and applying an electric field to the electrode to etch the convex portion present on the surface of the electrode. Barrel polishing is a method in which the surface is smoothed by mechanically pressing the convex portion of the surface.
However, although a technique for smoothing the surface of an electrode by polishing it using such a method as the above-mentioned electrolytic polishing method, barrel polishing method, or composite electrolytic polishing method is conventionally known, it was not known that the blackening of a quartz glass bulb due to the generation of sputtering of an electrode may be prevented if the Rmax value of the end portion of the electrode is less than a certain value. Also, it was not known that a blowout of a high pressure discharge lamp may be prevented if the Rmax value of portions of the electrode other than the end portion thereof is within a certain range.
In this specification, the term “an end of an electrode” indicates an end of an electrode along the length thereof which faces an opposite electrode side. The term “an end portion of the electrode” means the portion of the electrode which contributes to the discharge by the electrode and the portion may be expressed by the length between the end of the electrode and a certain distance away from the end of the electrode along the length thereof. The length may vary in accordance with the electric power supplied to the high pressure discharge lamp. More specifically, it is preferable, when the electric power supplied to the high pressure discharge lamp is expressed by P (in W), that the length be in the range between about P/150 and P/100 (in mm). That is, for instance, the length is 0.8–1.2 mm when P=120 W, 1.2–1.8 mm when P=180 W, and 1.33–2.0 mm when P=200 W. Note that if the anode and the cathode have the same shape, the above length is the same for the end portion of each of the electrodes. However, if the shapes of the electrodes are different, the lengths of the respective end portions are also different.
In the present invention, it is essential that the Rmax value of an end portion of an electrode be about 5 μm or less. If the Rmax is about 5 μm or less, it becomes possible to significantly reduce sputtering of an electrode in comparison with a conventional electrode and to prevent problems such as the blackening of a quartz glass bulb even after being lit for a considerably long time (for instance, more than 2,000 hours). According to the present invention, the smaller the Rmax of an end portion of an electrode, the greater the effect in reducing sputtering of the electrode. The Rmax of an end portion of an electrode is preferably about 3 μm or less, more preferably about 1 μm or less, and most preferably about 0.5 μm or less. If the Rmax of an end portion of an electrode is about 1 μm or less, problems associated with a quartz glass bulb such as the blackening of the bulb may be prevented even after being lit for more than 3,000 hours.
According to the present invention, the Rmax, of portions of an electrode other than the end portion thereof is preferably in the range between about 5 and 12 μm, and more preferably in the range between about 7 and 9 μm. When a high pressure discharge lamp is produced, a quartz glass is heated to a certain temperature so that an electrode may be sealed at a sealing portion of the quartz glass. After that, the quartz glass is cooled down, and a substantial solidification of the quartz glass is started at about the annealing temperature thereof. At that time, if the Rmax of portions of an electrode other than the end portion thereof is in the range between about 5 and 12 μm, the electrode and the quartz glass is tightly sealed to prevent a blowout of the high pressure discharge lamp even after being lit for a considerably long time (for instance, more than 2,000 hours). Also, if the Rmax is in the range between about 7 and 9 μm, it becomes possible to prevent a blowout of the high pressure discharge lamp even after being lit, for instance, for more than 2,500 hours. In this specification, the term “portions of an electrode other than the end portion thereof” means the portions of an electrode located in an expanded portion for luminescence of the quartz glass bulb, i.e., the portions of the electrode separated from the quartz glass bulb, other than the end portion and the contacting portion of the electrode.
According to the present invention, mercury vapor is contained in the high pressure discharge lamp. The amount of the mercury vapor is preferably in the range between about 0.12 and 0.3 mg/mm3, and more preferably in the range between about 0.18 and 0.24 mg/mm3. If the amount of the mercury vapor is in the range between about 0.12 and 0.3 mg/mm3, the luminous efficacy of the high pressure discharge lamp may be enhanced, and the generation of blackening or a blowout during its operation may be prevented.
According to the present invention, a halogen gas is contained in the high pressure discharge lamp. The amount of the halogen gas is preferably in the range between about 10−8 and 10−2 μmol/mm3, and more preferably in the range between about 10−6 and 10−4 μmol/mm3. If the amount of the halogen gas is in the range between about 10−8 and 10−2 μmol/mm3, the luminous efficacy of the high pressure discharge lamp may be enhanced and the generation of blackening or a blowout during its operation may be prevented. Examples of the halogen gas which may be used in the present invention include chlorine gas, bromine gas, and iodine gas, and one or more of these gases may be contained in the lamp. If more than two species of gases are contained, it is preferable that the total amount of the gases be in the range between about 10−8 and 10−2 μmol/mm3.
According to the present invention, an inert gas is contained in the high pressure discharge lamp. The pressure of the inert gas in the lamp is preferably about 6 kPa or more, and more preferably in the range between about 20 and 50 kPa If the pressure of the inert gas is about 20 kPa or more, the luminous efficacy of the high pressure discharge lamp may be enhanced and the generation of blackening or a blowout during its operation may be prevented. Examples of the inert gas which may be used in the present invention include helium gas, neon gas, argon gas, krypton gas, and xenon gas, and one or more of these gases may be contained in the lamp. If more than two species of inert gases are contained, it is preferable that the total pressure of the gases be about 50 kPa or less.
According to the present invention, the bulb wall loading in the high pressure discharge lamp is preferably about 0.8 W/mm2 or more, and more preferably in the range between about 1.2 and 1.8 W/mm2. If the bulb wall loading is about 0.8 W/mm2 or more, the luminous efficacy of the high pressure discharge lamp may be enhanced and the generation of blackening or a blowout during its operation may be prevented.
According to the present invention, the materials used for an anode and a cathode are preferably tungsten, molybdenum, and tantalum. The use of tungsten is more preferable and that of tungsten containing potassium oxide is especially preferable. The amount of potassium oxide in tungsten is preferably about 30 ppm or less. If tungsten containing potassium oxide is used, the luminous efficacy of the high pressure discharge lamp may be enhanced and the generation of blackening or a blowout during its operation may be prevented.
According to the present invention, the method for making or polishing an end portion of an electrode is not particularly limited as long as it can achieve the Rmax of the end portion 5 μm or less. Examples of such methods include an electrolytic polishing method and a composite electrolytic polishing method. It is preferable to employ the composite electrolytic polishing method since it can achieve the polishing of an electrode in an accurate and efficient manner.
The characteristics of an embodiment of the high pressure discharge lamp according to the present invention are described as follows:
The high pressure discharge lamp according to the present invention may be used in the same manner as a conventional high pressure discharge lamp. That is, when the high pressure discharge lamp of the present invention is connected to a power source, a trigger voltage is applied to the cathode and the anode in order to start the discharge. In this manner, a desired brightness of the lamp may be obtained. Also, according to the present invention, it becomes possible to provide a high pressure discharge lamp which, even after being lit for a considerably long time, does not have problems such as a blowout of the bulb made of quartz glass or the blackening of the quartz glass bulb.
Next, the present invention will be described in more detail with reference to particular embodiments. However, the present invention is not by any means to be restricted to the following embodiments.
Embodiments 1–3 and Comparative Embodiment 1
Using a high pressure discharge lamp having a structure as shown in
As a result, the time required for each of the high pressure discharge lamps to be blackened was 3,000 hours in Embodiment 1, 2,650 hours in Embodiment 2, 2,200 hours in Embodiment 3, and 1,000 hours in Comparative Embodiment 1 and it was confirmed that if the Rmax of the end portion of the electrode is 5 μm or less, the time required for the lamp to be blackened may be extended to 2,000 hours or more. The high pressure discharge lamp in Embodiment 1, whose Rmax value was 0.5 μm was the most excellent at exhibiting such an effect.
Embodiments 4–6 and Comparative Embodiments 2 and 3
The time required for the generation of a crack after lighting a high pressure discharge lamp was measured by using the same conditions as in Embodiment 1, except that the Rmax value for portions other than the end portion of the electrode was 3 μm for the high pressure discharge lamp in Comparative Embodiment 2, 6 μm for the lamp in Embodiment 4, 8 μm for the lamp in Embodiment 5, 10 μmm for the lamp in Embodiment 6, and 14 μm for the lamp in Comparative Embodiment 3.
As a result, all of the high pressure discharge lamps in Embodiments 4–6 were capable of extending the time needed for the generation of a crack to more than 2,000 hours. Among them, the high pressure discharge lamp in Embodiment 5, whose Rmax value was 8 μm had the most excellent effect. On the other hand, the time required for the generation of a crack of the lamps in Comparative Embodiments 2 and 3 were 1,800 and 1,500 hours, respectively, and these lamps could not extend the time required for the generation of a crack.
Having thus described exemplary embodiments of the invention, it will be apparent that various alterations, modifications, and improvements will readily occur to those skilled in the art. Such alterations, modifications, and improvements, though not expressly described above, are nonetheless intended and implied to be within the spirit and scope of the invention. Accordingly, the foregoing discussion is intended to be illustrative only; the invention is limited and defined only by the following claims and equivalents thereto.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2000-069172 | Mar 2000 | JP | national |
| 2000-242998 | Aug 2000 | JP | national |
The present Application is a Continuation Application of U.S. patent application Ser. No. 09/803,655, filed on Mar. 12, 2001 now U.S. Pat. No. 6,759,806.
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| Number | Date | Country | |
|---|---|---|---|
| 20040135512 A1 | Jul 2004 | US |
| Number | Date | Country | |
|---|---|---|---|
| Parent | 09803655 | Mar 2001 | US |
| Child | 10743070 | US |
