1. Field of the Invention
The present invention relates to a radiation generating apparatus in which a radiation tube is enclosed in an envelope filled with an insulating liquid.
2. Description of the Related Art
A radiation tube, which is a vacuum tube consisting of a cathode, an anode and an insulating tubular side wall, accelerates an electron emitted from an electron source of the cathode by high voltage applied between the cathode and the anode, irradiates a metal target provided on the anode with the accelerated electron, and thus generates a radiation. In a radiation generating apparatus in which the radiation tube like this has been enclosed in an envelope filled with an insulating liquid, the target is heated by the irradiation of the electron, the heat generated from the target is conducted to the peripheral insulating liquid, and the temperature of the insulating liquid is thus increased. Consequently, there are fears that the insulating liquid is deteriorated due to the increase of the temperature, and withstand voltage is thus decreased. For this reason, it is necessary to suppress or control the increase of the temperature of the insulating liquid by rapidly radiating the heat conducted to the insulating liquid. For example, each of Japanese Patent Application Laid-Open Nos. 2002-175899 and 2004-022459 discloses a technique of cooling an insulating liquid by providing an exothermic fin on the outer side of an envelope of a radiation generating apparatus and an endothermic fin on the inner side of the envelope thereof.
In the conventional structure, the endothermic fin is arranged on the inner side of the envelope so as to substantially face the whole area expanding from the cathode to the anode of the radiation tube. Since the potential of the envelope of the radiation generating apparatus is usually set to be the ground potential, a so-called electric field concentration comes to occur easily depending on the potential to be applied to the radiation tube. In general, when the electric field concentration occurs, the potential of the endothermic fin becomes relatively low in regard to the radiation tube. In such a case, to secure the withstand voltage, it is necessary to have a reasonable distance in the radiation tube as compared with a case where there is no endothermic fin, whereby such a circumstance becomes a barrier to achieve downsizing.
Consequently, an object of the present invention is to provide a radiation generating apparatus which is equipped with a cooling structure having an insulating liquid in the envelope thereof, and can secure the withstand voltage and downsize the entire apparatus.
In order to solve such conventional problems as described above, in the present invention, there is provides a radiation generating apparatus in which a radiation tube that a tubular side wall of a dielectric is arranged between a cathode having an electron-emitting device and an anode on which a target for generating a radiation in response to irradiation of an electron emitted from the electron-emitting device is provided is enclosed in an envelope which is filled with an insulating liquid, wherein a thermally-conductive fin projecting to a barrel portion of the radiation tube is provided on at least a part of an inner surface of the envelope, and the fin is provided on an area except for an area facing a position of the barrel portion at which potential of the barrel portion is higher than potential of the fin.
Moreover, in the present invention, there is provided a radiation generating apparatus in which a radiation tube that a tubular side wall of a dielectric is arranged between a cathode having an electron-emitting device and an anode on which a target for generating a radiation in response to irradiation of an electron emitted from the electron-emitting device is provided is enclosed in an envelope which is filled with an insulating liquid, wherein a thermally-conductive fin is provided on at least a part of an inner surface of the envelope so as to project to a barrel portion of the radiation tube, and, as a potential difference between the fin and the barrel portion becomes large, a distance between the fin and the barrel portion becomes large.
According to the present invention, the thermally-conductive fin absorbs the heat from the insulating liquid and conducts the absorbed heat to the envelope, thereby radiating the excessive heat to the outside through the envelope. Thus, it is possible to rapidly cool the insulating liquid. Moreover, the fin is provided so as to be able to suppress the decrease of the withstand voltage even if the distance between the fin and the barrel portion of the radiation tube is made small. Thus, it is possible to secure the withstand voltage, and it is also possible to downsize the entire apparatus.
Further features of the present invention will become apparent from the following description of the exemplary embodiments with reference to the attached drawings.
Hereinafter, exemplary embodiments of a radiation generating apparatus according to the present invention will be described in detail with reference to the attached drawings. Here, it should be noted that materials, dimensions, shapes, relative arrangements and the like of the constituent members described in the following exemplary embodiments do not limit the scope of the present invention, unless otherwise described. Also, it should be noted that X-rays are suitable as the radiation to be used in the present invention.
The constitution of the radiation generating apparatus according to the present invention will be described with reference to
A radiation generating apparatus 1 is formed by enclosing a radiation tube 2 in an envelope 3 together with an insulating liquid 4. Any of a reflection type radiation tube and a transmission type radiation tube can be used for the radiation tube 2, and a radiation transmission window (not illustrated) may be provided at the envelope 3 in accordance with a radiating position of the radiation tube 2.
Hereinafter, the structure of a transmission type radiation tube to be used for the radiation generating apparatus according to the present invention will be briefly described.
The radiation tube 2 is a vacuum tube formed by sealing a cathode 5, an anode 6 and a tube 7 composed of a dielectric substance (hereinafter, referred to as “tubular side wall 7”), which is arranged between the cathode and the anode. An electron gun structure having an electron-emitting device is connected to the cathode 5. The electron gun structure, which is potentially defined on the basis of potential of the cathode 5, is arranged inside the radiation tube 2. This electron gun structure is mainly composed of an electron source 11, a grid electrode 12 and a focusing electrode 13. A target 14, which generates a radiation by the irradiation of electrons emitted from the electron-emitting device, is provided at the anode 6. The voltage, which is about from several tens kV to several hundred kV, is applied to this anode 6. Although there are not many restrictions about a shape of the tubular side wall 7, a cylindrical form is preferable if considering about the miniaturization or easiness in manufacturing. However, for example, a horn tube or the like other than the cylindrical form is also available. In
The envelope 3, which is composed of a container unit 8 and a cover unit 9, is formed by fixing the radiation tube 2 to the container unit 8 and sealing the container unit with the cover unit 9. As the materials of the envelope 3, metals such as iron, stainless, lead, brass, copper and the like can be used. The insulating liquid 4 can be injected into the envelope 3 from a filler hole (not illustrated) provided at a part of the envelope 3. It is preferable that a potential of the envelope 3 is defined to become the ground potential.
It is preferable that the insulating liquid 4 has high electric insulation and a high cooling capacity. In addition, the insulating liquid, of which the quality is little changed by the heat, is preferable. For example, an electric insulating oil, a fluorinated insulating oil or the like can be used.
When the above radiation generating apparatus is operated, the radiation tube 2 (particularly, the anode 6) generates the heat, and that heat increases a temperature of the insulating liquid 4. Furthermore, there occurs such a convection flow of the insulating liquid 4 which moves toward a portion, where a potential is lower than an anode potential, mainly from the anode 6. Since the insulating liquid 4 thermally expands by the rise of temperature, there is some fear of damaging the envelope 3 (for example, leakage of liquid from a sealing portion between the container unit 8 and the cover unit 9). In addition, the insulating liquid 4 is deteriorated by the rise of temperature, and there is some fear of decreasing the withstand voltage. Therefore, a fin 10, which has thermal conductivity and projected to a barrel portion side of the radiation tube 2, is provided at least at a part of an inner surface of the envelope 3. It is preferable that a potential of the fin 10 is defined to become the ground potential. The fin 10 absorbs heat from the insulating liquid 4 and emits the heat to the outside of the envelope 3 by thermally conducting the heat to the envelope 3. It is preferable that a shape of the fin 10 is a slit-like form as illustrated in
By the way, when the fin 10 is provided at an inner surface of the envelope 3, there is some fear of decreasing the withstand voltage between the fin 10 and a barrel portion of the radiation tube 2 by the potential difference between the radiation tube 2 and the fin depending on a position. The decreasing of the withstand voltage causes the size increasing of the envelope 3, and this fact becomes an obstacle of the miniaturization. Since the electric field concentration tends to occur easily at a tip of the fin 10 as compared with a plane, electrons tend to be more easily emitted from a tip of the fin 10 to the side of the radiation tube 2 in a region of (the potential of the fin 10<the potential of the radiation tube 2) than a region of (the potential of the fin 10>the potential of the radiation tube 2), and the emitted electrons are accelerated. For this reason, in the region of (the potential of the fin 10<the potential of the radiation tube 2), an electric discharge due to such a phenomenon, where electrons are emitted from a tip of the fin 10 then the electrons collide with the radiation tube 2, tends to easily occur. That is, in the region of (the potential of the fin 10<the potential of the radiation tube 2), the withstand voltage tends to be easily decreased. For example, in a case that fins 10, of which thickness is about 1 mm and cross sections of the tip have a semicircular form, are arranged with an interval of about 5 mm, the field intensity is increased to about the double intensity as compared with a case of a plane plate. Therefore, in the present invention, it is not required to increase the size of the envelope 3 by forming that the projecting length of the fins 10 from an inner surface of the envelope 3 is made to be uneven in accordance with the potential of a barrel portion of the radiation tube 2 which faces to the fins 10. Specifically, it is preferable to provide the fins 10 as follows.
When the fin 10 is provided at a position excepting a region which faces to a position of a barrel portion of the radiation tube 2 of which the potential becomes higher than the potential of the fin 10, since the region of (the potential of the fin 10<the potential of the radiation tube 2) is not appeared, the electric discharge hardly occurs. In this case, it is preferable to provide the fin 10 so as to increase a distance between the fin 10 and a barrel portion of the radiation tube 2 to become a long distance according as the potential difference between the fin 10 and a barrel portion of the radiation tube 2 becomes a large difference. By constituting like this, the filed intensity between the fin 10 and a barrel portion of the radiation tube 2 does not become large in the region of (the potential of the fin 10>the potential of the radiation tube 2) to be preferably resulted.
When the fin 10 is provided so as to increase a distance between the fin 10 and a barrel portion of the radiation tube 2 to become a long distance according as the potential difference between the fin 10 and a barrel portion of the radiation tube 2 becomes a large distance, the filed intensity between the fin 10 and a barrel portion of the radiation tube 2 does not become large to be preferably resulted. Further, in this case, it is preferable to provide the fin 10 so that the change of distance between the fin 10 and a barrel portion of the radiation tube 2 becomes more gradual at a side where the potential of a barrel portion of the radiation tube 2 becomes lower than the potential of the fin 10 than a side where the potential of a barrel portion of the radiation tube 2 becomes higher than the potential of the fin 10.
It is preferable to constitute that the shortest distance from a barrel portion of the radiation tube 2 to the fin 10 becomes equal to or longer than the shortest distance from the radiation tube 2 to the envelope 3. By constituting like this, the field intensity between the radiation tube 2 and the envelope 3 does not become large to be preferably resulted.
When the same potential is set to the fin 10 and the anode 6, since the potential of a barrel portion of the radiation tube 2 is lower than the potential of the fin 10, a restriction for the arrangement of the fin 10 is decreased, and it is allowed that the fin 10 is arranged only on the periphery of the anode 6 which acts as a heat source.
Since there is possibility that the insulating liquid 4 stays at corner portions or the like inside the envelope 3, a rectifying structure 16, which makes a flow of the insulating liquid 4 direct toward the fin 10, is allowed to be provided on the periphery of the anode 6.
The constitution of a radiation generating apparatus in this example is the same as that exemplified in the above embodiment (
The radiation generating apparatus 1 is formed by enclosing the radiation tube 2 in an envelope and filling the insulating liquid 4 into the envelope. The radiation tube 2 is a transmission type radiation tube which is formed by holding the tubular side wall 7 between the cathode 5 and the anode 6 and sealing these members (
The envelope 3 made of brass, of which a shape is a rectangular solid form, is composed of the cover unit 9 for one surface and the container unit 8 for a part other than the one surface, and the envelope was defined to become the ground potential. A packing material used for the sealing (not illustrated) is provided at a joint between the container unit 8 and the cover unit 9, which were sealed by fixing with screws. The radiation tube 2 was arranged so that the tubular side wall 7 becomes parallel with the cover unit 9. In addition, the fin 10, which projects to the barrel portion side of the radiation tube 2, was provided at a position excepting a region which faces to a position of a barrel portion of the radiation tube 2, of which the potential becomes higher than the potential of the fin 10, on an inner surface of the cover unit 9. The potential of the fin 10 is also equal to the ground potential. A tip of the fin 10 made of brass, of which thickness is 1 mm, is chamfered to have such a radius equal to 0.5 mm, and thirteen pieces of the fins are arranged with an interval of 4 mm. The shortest distance from a barrel portion of the radiation tube 2 to the fin 10 is made to become equal to or longer than the shortest distance from the radiation tube 2 to the envelope 3, and the field intensity between the radiation tube 2 and the envelope 3 is made not to become large. Although the field intensity of the tip of the fin 10 locally becomes high, since the potential of the fin 10 is higher than the potential of the radiation tube 2 at a position which faces to the fin 10, the electric discharge hardly occurs.
A high voltage insulating oil A (produced by JX Nippon Oil & Energy Corporation) is used for the insulating liquid 4, which is filled into the envelope from a filler hole (not illustrated) provided at the envelope 3.
As mentioned above, the field intensity is increased at a tip of the fin 10. In this example, the field intensity is increased to about the double intensity at the tip of the fin 10. According to this fact, if the fin 10 is provided at the whole region which faces to a barrel portion of the radiation tube 2 and the withstand voltage is intended to secure, the distance between the fin 10 and a barrel portion of the radiation tube 2 has to be increased to such a distance nearly equal to at least the shortest distance between the radiation tube 2 and the envelope 3. On the other hand, in the present embodiment, since the fin 10 is provided at a position excepting a region which faces to a position of a barrel portion of the radiation tube 2, of which the potential becomes higher than the potential of the fin 10, the shortest distance between the radiation tube 2 and the envelope 3 can be reduced to a short distance as compared with a case that the fin 10 is provided at the whole region which faces to a barrel portion of the radiation tube 2. Accordingly, the miniaturization of an apparatus can be realized by this example.
When the radiation generating apparatus 1 in this example was driven with the potential of −50 kV for the cathode 5 and the potential of 50 kV for the anode 6, a radiation could be generated without an obstacle due to the electric discharge. In addition, the damage of the envelope 3 such as an oil leakage or the like due to the increasing of temperature did not occur. Further, even if the apparatus has been driven for a long time, the electric discharge did not occur and the deterioration of the withstand voltage was not confirmed.
The constitution of a radiation generating apparatus 1 in this example is different from the constitution of the Example 1. The projecting length of the fin from the cover unit 9 is decreased according as the fin 10 approaches closer to the cathode 5 as illustrated in
In the Example 1, since the potential difference between the fin 10 and a barrel portion of the radiation tube 2 becomes a large difference according as the fin approaches closer to the cathode 5, the fin 10 and a barrel portion of the radiation tube 2 have to be separated each other by the required distance in the vicinity of the cathode 5. On the other hand, since the potential difference between the fin 10 and a barrel portion of the radiation tube 2 does not almost occur in the vicinity of an intermediate point between the cathode 5 and the anode 6, the distance between the fin 10 and a barrel portion of the radiation tube 2 can be shortened in the vicinity of the intermediate point. Therefore, the distance between the radiation tube 2 and the envelope 3 can be suppressed to the minimum distance by forming the fin 10 into a shape as in this example, and the apparatus can be further miniaturized than the miniaturization in the Example 1.
Since the endothermic effect is faded out by decreasing an area of the fin 10, an endothermic area is supplemented by providing the fin 15 on a surface opposite to the cover unit 9 in this example. Of course, the distance between the radiation tube 2 and the envelope 3 is not required to increase due to the fin 15.
When the radiation generating apparatus 1 in this example was driven with the potential of −50 kV for the cathode 5 and the potential of 50 kV for the anode 6, a radiation could be generated without an obstacle due to the electric discharge. In addition, the damage of the envelope 3 such as an oil leakage or the like due to the increasing of temperature did not occur. Further, even if the apparatus has been driven for a long time, the electric discharge did not occur and the deterioration of the withstand voltage was not confirmed.
The constitution of a radiation generating apparatus in this example is different from the constitution of the Example 2. As illustrated in
When the radiation generating apparatus 1 in this example was driven with the potential of −100 kV for the cathode 5, a radiation could be generated without an obstacle due to the electric discharge, and the increasing of temperature could be more suppressed as compared with a case of the Example 2.
In addition to a case of the Example 2, in a radiation generating apparatus in this example, a rectifying structure 16 for rectifying the insulating liquid 4 to direct toward the fin 10 was provided between the anode 6 and the envelope as illustrated in
When the radiation generating apparatus 1 in this example was driven with the potential of −50 kV for the cathode 5 and the potential of 50 kV for the anode 6, a radiation could be generated without an obstacle due to the electric discharge, and the increasing of temperature could be more suppressed as compared with a case of the Example 2.
While the present invention has been described with reference to the exemplary embodiments, it is to be understood that the invention is not limited to the disclosed exemplary embodiments. The scope of the following claims is to be accorded the broadest interpretation so as to encompass all such modifications and equivalent structures and functions.
This application claims the benefit of Japanese Patent Application No. 2011-270081, filed Dec. 9, 2011, which is hereby incorporated by reference herein in its entirety.
Number | Date | Country | Kind |
---|---|---|---|
2011-270081 | Dec 2011 | JP | national |