1. Field of the Invention
The present invention concerns a rotary piston x-ray tube.
2. Description of the Prior Art
Rotary piston x-ray tubes are known, for example, from U.S. Pat. Nos. 6,426,998 and 6,339,635. An anode formed as an anode plate is disposed opposite a cathode in these known rotary piston x-ray tubes. The anode forms a base of the piston of the rotary piston x-ray tube. In the operation of the rotary piston x-ray tube, an electron beam emanating from the cathode strikes a stationary focal spot in the edge region of the anode plate. By rotation of the piston, the focal spot describes a circular focal path on the anode plate.
The heat formed by the absorption of the electrons is dissipated to a coolant via the back side of the anode plate facing away from the cathode. Given a constant radiation capacity, the heating of the anode is primarily determined by the rotational spread of the rotary piston x-ray tube as well as by the radius of the focal path. The largest possible radius of the focal path is structurally limited by the diameter of the anode plate.
Increasing the radiation capacity of the rotary piston x-ray tube leads to an increased heat entry into the anode. Since the cooling capacity of the anode is limited, for example by the maximum rotational speed, the radiation capacity of the rotary piston x-ray tube cannot be increased without further measures.
The rotational speed frequency of the rotary piston x-ray tube is limited by its moment of inertia. The massively designed anode with the anode plate contributes a significant proportion of the moment of inertia. An increase of the rotational speed for reduction of the heating of the anode is possible only to a certain degree.
An object of the present invention is to avoid the aforementioned disadvantages of the prior art. In particular a rotary piston x-ray tube with improved cooling of the anode should is achieved. A further object is to provide a rotary piston x-ray tube with an increased radiation emission capacity, while improving the lifespan.
This object is achieved by a rotary piston anode tube wherein the anode forms a radially rotating section of a wall of the piston shell or housing. It is thereby possible to enlarge the radius and thus the length of the focal path. In particular the contact surface of the anode that faces the coolant is thereby enlarged. As a result, heat can be better dissipated from the anode, and therewith the radiation capacity of the rotary piston x-ray tube can be increased. In addition to this, the lifespan of the rotary piston x-ray tube can be increased.
Furthermore, the rotary piston x-ray tube can be constructed with a lower mass. Instead of a massively-fashioned anode, the shell wall of the piston can be used as a cooling body. As a result, the moment of inertia of the piston can be decreased. The maximum rotational speed can be increased and the cooling of the anode can be further improved. Apart from this, the length of the piston and thus the space requirement of the rotary piston x-ray tube can be reduced.
Furthermore, the base of the piston is not occupied by the anode. It is possible to utilize the base for functional purposes. In comparison with conventional rotary piston x-ray tubes, it is possible to modify or to improve the arrangement of components of the rotary piston x-ray tube. Additional components such as, for example, an arrangement for deflecting electron beam can be mounted on the base.
In an embodiment of the invention, the rotating section is located in the region of the maximum radius of the shell wall. Heating of the focal path and thermal loading of the anode can thereby be reduced and the lifespan of the rotary piston x-ray tube increased. Sections of the shell wall can advantageously be provided with smaller radii than the maximum radius. A rotary piston x-ray tube with smaller moment of inertia can be rotated with a higher rotational speed. The cooling of the anode and of the focal ring can be improved.
In a further embodiment, the shell wall has a frustrum-shaped region. The shell wall can also have a cylindrical region. The regions are particularly simple geometric shapes for the manufacture of the shell wall. Cylindrical regions with different radii can also be connected by frustrum-shaped regions. Pistons thus can be produced with optimally small moment of inertia.
According to a further embodiment of the invention, the anode can be cylindrical or frustrum-shaped. Rotary piston x-ray tubes with different angles of incidence of the electron beam on the anode thus can be produced. Furthermore, it is possible to vary the irradiation direction of the x-ray radiation by a suitable geometry of the anode. For example, rotary piston x-ray tubes can be produced that radiate x-ray radiation in a direction parallel to the rotational axis or also a direction at an angle thereto. The frustrum is thereby opened in the direction parallel to the axis. If the frustrum is opened opposite to this direction, a rotary piston x-ray tube can be produced that radiates x-ray radiation in the opposite direction.
In another embodiment of the invention, the shell wall is cooled at its exterior. The shell wall can be cooled as a whole or only in the region of the anode. The cooling can be a direct cooling in which the exterior is charged with a coolant such as a liquid. The heat dissipation can be improved by utilization of the rotation of the piston. The exterior surface can be enlarged by a co-rotating structure, for example grooves, webs and the like on the exterior surface of the shell wall, the exterior surface can be advantageously enlarged, the coolant can be circulated and an improved heat dissipation can be achieved. An effective cooling enables the maintenance intervals as well as the lifespan of the rotary piston x-ray tube to be lengthened.
According to a further embodiment, a section of the piston has a focusing element for focusing the electron beam emanating from the cathode. The focusing element is preferably mounted on the base of the piston. A more precise focusing of the electron beam thus can be achieved. The radiation pattern of the x-ray radiation can be improved.
According to a further embodiment, the anode has a layer made from a high-melting-point material. Such materials exhibit melting points up to approximately 4000° C. Materials such as, for example, graphite preferably are used. The anode can furthermore have an x-ray-emissive layer that, for example, can be produced from Wo, Mo, Re or a Wo—Rh alloy. The characteristic (such as, for example, the wavelength or characteristic radiation) of the x-ray radiation can be established by the x-ray-emissive layer. The remaining part of the anode can be produced from a good heat-dissipating material that can be connected in a simple manner with the material of the shell wall and the x-ray-emissive layer. The anode preferably exhibits a thickness in the range of 10 to 20 mm; the x-ray-emissive layer preferably exhibits a thickness in the range of 0.5 mm to 1.5 mm. Such thicknesses are sufficient to prevent a melting of the materials by the electron beam and to ensure an optimally complete absorption of the electrons and a best-possible conversion of the energy of the electrons into x-ray radiation.
According to a further embodiment of the invention, the shell wall has a section produced from aluminum. Aluminum is particularly well-suited for manufacture of the shell wall of the piston. It exhibits a low atomic mass and a high heat conductivity. Furthermore, the shell wall can be produced from a non-magnetic material. Non-magnetic materials such as, for example, aluminum or stainless steel are particularly suited for rotary piston x-ray tubes in which the electron beam is deflected by electromagnetic fields. Non-magnetic materials do not interfere with the magnetic field that is externally applied to the piston for deflection of the electron beam, and allow an exact deflection of the electron beam. By a suitable selection of the materials for manufacture of the shell wall, its properties can be adapted to the requirements for a specific use of the rotary piston x-ray tube. For example, by the use of stainless steel the mechanical stability of the shell wall can be improved. Materials with good heat conductivity, for example aluminum, are particularly suited for production of pistons with small moments of inertia. These can be rotated with a higher rotational speed, so the cooling of the anode can be improved. The thickness of the shell wall is preferably in the range between 1 mm and 3 mm.
According to a further embodiment, the anode extends only over a segment of the thickness of the shell wall. The heat can be dissipated at the externally cooled shell wall. The heat dissipation from the anode to the shell wall can be increased by an optimally good coupling, for example with a heat conduction paste.
The anode can be inserted into a groove located on the inside of the shell wall. The manufacture of the rotary piston x-ray tube, in particular the fixing of the anode in the piston, can thereby be simplified.
The operation of the rotary piston x-ray tube of
During operation of the rotary piston x-ray tube, an electron beam 10 emanates from the cathode 2 located in the vacuum-sealed piston 1. Electromagnetic fields generated by a beam deflector arrangement (not shown), deflect the electron beam 10 such that it strikes the approximately 1 mm-thick, x-ray-emissive first layer 11 (produced, for example, from Wo, Mo or Re) of the first anode 3a. The electron beam 10 strikes on the first layer 11 in a focal spot (not designated) that is stationary relative to the rotational axis A. Due to the rotation of the piston 1 of the rotary piston x-ray tube, the focal spot describes a focal path on the first layer 11. Heat is generated by absorption of electrons of the electron beam 10, causing the first anode 3a to become substantially elevated in temperature. The heat is dissipated via the second layer 12 (for example, approximately 2 mm thick, produced from graphite) to the outer surface 14 of the piston 1. The outer surface is charged with a coolant (not shown) and is thereby directly cooled. The focal path is located in a region with the maximum radius of the piston 1. The first radial distance M corresponds to the maximum radius of the piston 1. A largest-possible length and area of the focal path thereby result. The temperature and the thermal loading of the anode 3a and of the bordering material (for example produced from aluminum or stainless steel) and the shell wall 5 are reduced. The lifespan and the maintenance intervals of the rotary piston x-ray tube can be increased.
The shell wall 5 includes the frustrum-shaped section 8 and the second cylindrical section 9b. Both sections 8 and 9b are closer to the rotational axis A than the first cylindrical section 9a containing the anode 3a. The moment of inertia of the piston 1 can be minimized by designing the shell wall 5 to the rotational axis A. The rotational speed of the piston 1 can be increased, and thus the focal ring temperature can be reduced.
The rotation of the piston 1 can be utilized in order to achieve an optimally good contact and heat transfer between the outer surface 14 and the coolant. Furthermore, the outer surface can be structured, for example with grooves or webs. The outer surface 14 effectively available for cooling can thereby be enlarged. Moreover, with a suitably-structured outer surface 14 it is possible to optimally circulate the coolant by utilizing the rotation and to achieve an optimally advantageous dissipation of the heat. The anode 3a including the focal path is cylindrically fashioned in the shown rotary piston x-ray tube. The emission of the x-ray radiation 13 ensues in the x-direction essentially parallel to the rotational axis A. The aperture angle of the emitted x-ray radiation 13 is determined by the angle of incidence of the electrons on the x-ray-emissive first layer 11. The radiation is itself limited in the y-direction by the anode 3a.
The deflection arrangement (not shown) for deflection of the electron beam 10 can be mounted on the first piston base 7 not occupied by the anode 3a. Such deflection arrangement enables a particularly precise positioning of the focal spot.
In
In the rotary piston x-ray tube shown in
Such a piston 1 is particularly simple to manufacture. No cylindrical sections need to be manufactured for the shell wall 5. The shell wall 5 has a more stable structure. Furthermore, in comparison with
The dimensions of the shell wall 5 of the rotary piston x-ray tube of
In the rotary piston x-ray tube of
BF5=2π*H*B
results for the focal ring area BF5 of
BF1=2π*M*B
for the focal ring area of
A negligible enlargement of the radius of the focal spot from the rotational axis A, for example from the second radial separation H of the conventional rotary piston x-ray tube to the radial separation M of the inventive rotary piston x-ray tube already leads to a significant enlargement of the focal ring area. For example, if H=10 cm, M=11 cm and B=2 mm, the area of the focal ring can be enlarged by approximately 10%. Associated with this is a reduction of the focal ring temperature and the thermal load of the anodes 3a through 3d. It is in particular possible to increase the capacity of the rotary piston x-ray tube with the same thermal load.
In comparison to the conventionally-arranged anode of
Although modifications and changes may be suggested by those skilled in the art, it is the intention of the inventor to embody within the patent warranted hereon all changes and modifications as reasonably and properly come within the scope of his contribution to the art.
Number | Date | Country | Kind |
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10 2004 030 832.2 | Jun 2004 | DE | national |