Patent Application
20210210336
The present invention relates to a high-pressure discharge lamp having a cathode made of tungsten or tungsten alloy, and more particularly to a high-pressure discharge lamp applied to the light source of a cinematographic projector, the light source used for exposure purposes in semiconductor or liquid crystal production fields, or to the light source used in analysis applications.
High-pressure discharge lamps are used for digital cinema projectors, exposure devices, and light sources in analysis applications in combination with an optical system as a light source with high light collection efficiency, because of its nature similar to a point light source due to the short distance between the tips of a pair of electrodes arranged opposite each other inside an arc tube.
A xenon lamp for use in a digital projector described in JP-A-2012-150951 (Patent Document 1) is one example of such high-pressure discharge lamps.
A cathode lead rod 22 and an anode lead rod 32 are respectively inserted into the cathode 21 and the anode 31. The cathode lead rod 22 and the anode lead rod 32 are sealed by sealing parts 13 of the sealed tubes 12.
As illustrated in
The example illustrated in
The OH group contained in the inner surface layer of the fused quartz light-emitting part 11 is released into the discharge space S as water (H2O), for example, during the illumination of the lamp. The released H2O reacts with carbon or carbon compound of the tungsten carbide layer 40 provided on the surface of the cathode 21 in the light-emitting part 11 mainly on the cathode surface, as a result of which carbon monoxide gas (CO) is generated.
This CO in the gaseous state diffusing inside the discharge space S of the light-emitting part 11 partly enters the arc A. Inside the arc A, the CO is heated and decotnposed so that C+ ions are generated. The generated C+ ions are transported toward the tip of the cathode by the electric fields inside the arc A, where the ions react with the tungsten W of the cathode 21 and form tungsten carbides such as W2C and WC.
The tungsten carbide formed on the surface at the tip of the cathode melts on the surface of cathode tip by the heat, in particular, when the lamp is turned on so that the surface of cathode tip is maintained smooth. This prevents formation of irregularities on the surface of cathode tip and allows for stable discharge.
Cathodes of such high-pressure discharge lamps, in particular xenon short arc lamps for use in digital projectors, are sometimes used under very harsh conditions with high operating pressure and high current density at the cathode tip.
Continuous illumination under these conditions leads to deformation and irregularities of the cathode tip, which causes the discharge point to move around (arc-jump), and thus flickering starts. This is because the carbon in the tungsten carbide (W2C) layer 40 decreases with the progress of time in which the lamp is illuminated, which makes the series of reactions illustrated in
Namely, the decrease in carbon C in the tungsten carbide (W2C) layer 40 leads to reduction of carbon monoxide CO in the discharge space S of the light-emitting part 11 and reduction of C+ ions in the arc, because of which tungsten carbides such as W2C and WC are formed less or not formed at all at the tip of the cathode 21. This causes formation of irregularities on the surface of cathode tip, resulting in the start of flickering.
Patent Document. 1: JP-A-2012-150951
In view of the issue in the prior art described above, one problem to be solved by this invention is to provide a high-pressure discharge lamp which includes a cathode body composed of the cathode made of tungsten or tungsten alloy, and a lead rod inserted in a lead rod insertion hole of this cathode; and that has a long service life wherein, after the lamp is turned on, formation of irregularities on the surface of the cathode tip is prevented and the flickering phenomenon is prevented from occurring for a long time.
To solve the above problem, the high-pressure discharge lamp according to this invention is characterized in that the cathode has a carbonized layer formed on a surface thereof exposed to a discharge space (except for a tip portion thereof) and on an inner surface of the lead rod insertion hole.
The carbonized layer is made of tungsten carbide (W2C).
The carbonized layer has a thickness of 20 to 40 μm.
In the high-pressure discharge lamp according to this invention, a carbonized layer is formed on surfaces of the cathode exposed to the discharge space so that carbon is diffused not only from the surface in the tip portion of the cathode but also from the surface in a rear end portion to maintain generation of CO on the cathode surface.
Moreover, the carbonized layer formed also on the inner surface of the lead rod insertion hole allows for carbon diffusion from inside of the cathode toward the surface during illumination, which makes it possible to sustain generation of CO on the cathode surface for a long time. The sustained generation of CO maintains the level of carbon monoxide CO in the light-emitting part so that the amount of C+ ions in the arc is maintained. Formation of tungsten carbides such as W2C and WC at the tip of the cathode 2 consequently prevents generation of irregularities at the tip of the cathode and as a result the service life before flickering starts can be prolonged.
The tungsten may contain impurities as much as would be mixed in during the refining process of tungsten. The tungsten alloy is an alloy of tungsten W and thorium oxide ThO2, or the oxide of rare earths such as cerium Ce and lanthanum La. The alloy may contain intermetallic compounds between these oxides and tungsten.
The cathode body 1 may be formed by joining tungsten and tungsten alloy together.
As described above, the carbonized layer 5 is formed on surfaces of the cathode 2 exposed to the discharge space. In so far as the effect of the present invention is achieved, there may be parts where no carbonized layer is provided, or where the carbonized layer is thin.
In the case of using tungsten carbide for this carbonized layer 5, the carbonized layer should preferably contain carbon C in an amount of 0.44 to 0.53 g/cc.
Too large an amount of carbon C would lead to excessive generation of CO on the cathode surface, which will cause the carbon C to be transported not only to the surface of the cathode tip but also to the surface of the anode tip, where tungsten carbides such as W2C and WC will be formed. Since the surface of anode tip is heated to a higher temperature than the surface of cathode tip during the time when the lamp is illuminated, the carbides on the surface of anode tip will vaporize, which leads to unwanted acceleration of blackening of inner surfaces of the discharge vessel.
On the contrary, too small an amount of carbon C would lead to early irregularities of the tip of the cathode due to insufficient generation of CO on the cathode surface, which allows the arc discharge point to move more easily and causes flickering.
The carbonized layer 5 should preferably have a thickness of 20 to 40 μm.
Too large a thickness of the carbonized layer would lead to excessive generation of CO on the cathode surface, which will cause the carbon C to be transported not only to the surface of the cathode tip but also to the surface of the anode tip, where tungsten carbides such as W2C and WC will be formed. These carbides vaporize and accelerate blackening of inner surfaces of the discharge vessel.
Too small a thickness of the carbonized layer would lead to early irregularities of the tip of the cathode due to insufficient generation of CO on the cathode surface, which causes flickering.
This carbonized layer 5 is not formed to the tip portion 2a of the cathode 2. Thoriated tungsten which is the material of the cathode 2 has a melting point of 3420° C., while the substances that form the carbonized layer 5 have a lower melting point than that (for example, the melting point of tungsten carbide is about 2800° C.). If the carbonized layer 5 is formed to the tip portion 2a of the cathode 2, the carbonized layer 5 on the tip portion 2a will melt excessively during the illumination, leading to earlier occurrence of the flickering.
This is why the carbonized layer 5 is not formed at the point where it will reach a temperature at which it melts, i.e., the tip portion 2a. Specifically, the carbonized layer 2 is not formed in an area of 3 to 5 mm from the tip in the case of a xenon lamp of about 2 to 6 kW.
In the present invention, the carbonized layer 5 is formed also on inner surfaces of the lead rod insertion hole 3 of the cathode 2.
As illustrated in
This carbon C diffused from the lead rod insertion hole 3 into the electrode gradually reaches the cathode surface and contributes to the generation of CO on the cathode surface.
The inner surface temperature of this lead rod insertion hole 3 is lower than the temperature on the surface of the cathode, because of which the carbon diffusion from the carbonized layer 5 of the lead rod insertion hole 3 and from the carbonized layer 5 of the cathode surface occur with a time difference. This allows the carbon to be replenished at about the time when carbon in the carbonized layer 5 on the cathode surface is consumed and reduced, so that depletion of carbon in the carbonized layer 5 on the cathode surface is inhibited.
In so far as the effect of the present invention is achieved, there may be parts where no carbonized layer is provided, or where the carbonized layer is thin, on the inner surface of the lead rod insertion hole 3.
For the formation of such a carbonized layer 5, a gas-phase carbonization method may be utilized. The gas-phase carbonization is a method wherein a mixture gas of benzene and hydrogen is made to react with the cathode heated in a high-frequency heating device.
A process gas which is a mixture of benzene and hydrogen is supplied to a reaction chamber to flow at a rate of about 2 L/min. The cathode inside the reaction chamber is heated to about 1900° C. by high-frequency heating and kept at the high temperature for 5 minutes. The mixture gas is replaced with hydrogen gas, the temperature is reduced to about 1;%00° C. and this temperature is maintained for 5 minutes. This process is repeated several times until a cathode body with a carbonized layer of about 30 μm formed thereon is obtained.
The carbonized layer 5 is thus formed entirely on outer surfaces of the cathode 2 as well as on inner surfaces of the lead rod insertion hole 3. After that, the carbonized layer is removed by a machining process from the tip portion 2a of the cathode 2.
In the high-pressure discharge lamp according to this invention, a carbonized layer is formed on the surface of the cathode exposed to the discharge space (except for the tip portion) to maintain generation of CO on the cathode surface. Moreover, the carbonized layer formed on the inner surface of the lead rod insertion hole allows for carbon diffusion from inside of the cathode toward the surface during illumination which makes it possible to sustain generation of CO on the cathode surface over a long time.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2018-097692 | May 2018 | JP | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/JP2019/004358 | 2/7/2019 | WO | 00 |
