1. Field of the Invention
The invention relates to a short arc discharge lamp and a light source device using this lamp. The invention relates especially to an improvement of the starting properties of this short arc discharge lamp.
2. Description of the Related Art
In a short arc discharge lamp, in general, as shown in the schematic in
In the above described
A primary object of the present invention is to devise a short arc discharge lamp with a good starting property in which there is no danger of damaging the arc tube and in which the radiant light from the arc tube is not adversely affected.
A further object of the invention is to devise a light source device in which this discharge lamp is used and the focusing area is increased.
According to a first embodiment of the invention, a short arc discharge lamp is constructed having a discharge space surrounded by an arc tube in which a first high voltage electrode is situated to be at an electrical potential and spaced a distance from a second, opposite electrode. The objects of the invention are achieved by providing, in the discharge space, at least one conductive component with a tip projecting into the discharge space and having an electrical potential which is identical to the electrical potential of the first electrode. The tip is at a distance from the second electrode which is greater than the distance between the first and the second electrode.
The objects are also achieved by an embodiment of the invention where the tip of the conductive component is in contact with the inside wall of the arc tube or approaches the inside wall of the arc tube.
The objects of the invention are also achieved by a short arc discharge lamp having the conductive component located outside the area which lies around the electrode axis proceeding from the arc middle in the area of the light utilization angle.
The objects of the invention are still further achieved by a light source device in which one of the hermetically sealed portions of the above described short arc discharge lamp is pushed into the neck of a concave reflector.
The expression “short arc discharge lamp” of the invention is defined as a discharge lamp in which the added rare gas is Xe, Kr, or Ar or a gas mixture thereof, or a discharge lamp in which these gases are used as a buffer gas and in which mercury and/or at least one halogenated metal is added. The distance between the electrodes can be, for example, a few mm to roughly 10 and a few mm.
The area of the “light utilization angle” is the so-called light distribution angle. In
The conductive component is located in the discharge space outside the axis of the electrodes and has the same electrical potential as the electrode on the side to which the high voltage is applied. The high voltage is also applied to the above described electrical component, and the electrical field of the tip of this conductive component is locally intensified. The gas at this location reaches the breakdown voltage, by which ionization and a corona discharge (local discharge) form. In the lamp of the invention, it is assumed that the electromagnetic waves which are formed by the above described corona discharge induce electron emission from the cathode or the anode by the photoelectric effect. The breakdown voltage between the main electrodes is therefore reduced and thus the main discharge takes place.
The arrangement of the invention is such that the tip of the conductive component is located a distance from the electrode which is opposite the electrode to which the high voltage is applied and the distance is greater than the distance between the electrode receiving the high voltage and the electrode opposite it. Therefore, when the main discharge begins, the potential difference between the electrodes to which a few 10 kV have been applied during starting is lowered to a few dozen V, by which the field intensity at the start of ionization is not reached and by which the corona discharge is stopped.
In a high pressure rare gas discharge lamp which is represented by a xenon short arc discharge lamp, the filling pressure of the gas is high. At the tip of the conductive component, therefore, a corona discharge is easily limited. This can be an especially advantageous embodiment of the invention.
a) and 3(b) each show a schematic of one embodiment of the installation of a conductive component of the invention;
a) and 4(b) each show a schematic of another embodiment of the installation of a conductive component of the invention;
a) and 5(b) each show a schematic of still another embodiment of the installation of a conductive component of the invention;
a) and 10(b) each show a schematic of one example which confirms the action of the invention;
The connection methods for attaching the conductive component 15 is as follows:
If the material of the conductive component is a metal with a high melting point such as Mo, W, Ta, Zr and the like as the carrier (substrate) metal and if at least the tip area of this component contains a material with a low (electron) work function such as Th, La, Ce, Hf, Ba and the like, the discharge is started with a lower voltage than in the case in which only metals with a high melting point such as Mo, W, Ta, Zr and the like are contained.
As is shown in
Next, as a specific example of the invention, a high pressure xenon lamp for a DLP projector with an output wattage of 2 kW, a xenon fill pressure of 2 MPa, and a distance between the electrodes of 5 mm, is provided with a conductive component positioned within an arc tube. In one example, a molybdenum (Mo) line 27 is attached to a glass tube (
Test to Confirm the Starting Property
Two lamps at a time were produced with a conventional arrangement of the trigger wire outside the arc tube and with the above described three versions. The breakdown voltage was determined for them.
The result of measuring the breakdown voltage during the starting operation is described below. In the case of conventional winding of the trigger wire outside the arc tube the breakdown voltage of the lamps was 30 kV to 33 kV. Conversely, the breakdown voltage in the versions of the invention was 25 kV to 27 kV for first version and 22 kV to 24 kV for second and third versions. The breakdown voltage has therefore decreased to a large extent.
In the case of the three versions of the invention, there is no degradation of the conductive component by oxidation because the conductive component is located within the lamp. Therefore, the starting property is not degraded at the end of the lamp service life. The phenomenon which occurred in the arc tube for each version was the following:
In the first version, when a high voltage was applied to the tip of the Mo line 27 of the conductive component a discharge similar to fireworks formed. In the second and third versions, a discharge propagated from the tip of the conductive component to the inside wall of the bulb in the manner of a spider's web. It can be assumed that it was formed by a corona discharge passing from the discharge form into a creeping discharge along the inside of the glass.
From the aforementioned result the following can be assumed:
At a voltage (roughly 10 kV) which is lower than the breakdown voltage between the main electrodes, a corona discharge is formed proceeding from the tip of the Mo line. The electromagnetic waves which are produced by this discharge can induce electron emission by the photoelectric effect from the cathode or anode and thus can reduce the breakdown voltage between the main electrodes. When the main discharge begins, the potential difference between the electrodes to which a few 10 kV were applied during starting decreases to a few dozen V, such that the field intensity at the start of ionization is not reached and the corona discharge is stopped so that only the main discharge is continued.
In the description above, a lamp of the direct current type is shown by way of example. However, the conductive component inside is active independently of whether a direct current or alternating current is used, even if the lamp is started by applying a high voltage to the component in a lamp via an alternating current type. It can be imagined that the action of the invention is, of course, also achieved in doing by so starting the lamp.
As was described above, according to the first embodiment of the invention, a short arc discharge lamp is obtained with good starting property, in which there is no danger of damage to the arc tube by a trigger wire positioned outside the arc tube. In this first embodiment, in a short arc discharge lamp having a discharge space, there is a pair of electrodes opposite one another. In the discharge space, besides these electrodes there is at least one conductive component where the electrical potential of this conductive component is identical to the electrical potential of the electrode on the side to which the high voltage is applied. Further, the tip of the above described conductive component is at a distance from the electrode which is opposite the electrode to which the high voltage is applied, this distance being greater than the distance between the electrode on the high voltage application side and the electrode opposite it.
Furthermore, a short arc discharge lamp with an even better starting property can be obtained by the embodiment in which the tip of the conductive component is in contact with the inside wall of the arc tube or is close to it.
Additionally, a short arc discharge lamp, with high efficiency of light usage, is obtained in which the radiant light from the arc tube is not adversely effected by the conductive component located outside the area which extends around the electrode axis proceeding from the arc center in the effective light utilization angle.
Moreover, the light source device of the invention includes a device in which there is a concave reflector in which one of the hermetically sealed portions of the short arc discharge lamp is pushed into the neck of the concave reflector. In such an embodiment, a light source device with a short arc discharge lamp is obtained in which the diameter of the mirror opening can be made small and in which the focusing area is enlarged without adversely affecting the radiant light of the arc tube.
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2002-213298 | Jul 2002 | JP | national |
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