1. Field of the Invention
The present invention relates to radiographic equipment, and particularly, to an X-ray tube having a rotating and linearly translating anode.
2. Description of the Related Art
An X-ray tube is a vacuum tube that produces X-rays, typically found in medical X-ray machines and the like. As with any vacuum tube, there is an emitter, typically a filament cathode, which emits electrons into the vacuum, and an anode to collect the electrons, thus establishing a flow of electrical current, referred to as the “beam”, through the tube. A high voltage power source, for example 30 to 150 kV), is connected across the cathode and anode to accelerate the electrons. The X-ray spectrum produced depends on the anode material and the accelerating voltage.
Electrons from the cathode collide with a target deposited on the anode, with the target often formed from tungsten, molybdenum or copper. During collisions, the electrons lose energy in both collisional and radiative modes. About 1% of the kinetic energy during the collision process is converted into X-ray radiation. This is due to the deceleration of the electrons within the electrical field of the nucleus, or through the creation of vacancies in the inner shells of bound electrons.
Coolidge tubes are formed as either end-window tubes or side-window tubes. In an end-window tube, the filament is wrapped about the anode, so the electrons have a curved path. The tube 100 of
The rotating anode tube 200 is also a vacuum tube, formed from shell 202 having an X-ray window 210 formed therein. The anode 204 consists of a disc with an annular target 206 formed thereon. The anode disc 204 is supported on an axle 214, which is supported by bearings 212 within the tube shell 202. The anode 204 can then be rotated by electromagnetic induction from a series of stator windings outside the evacuated tube.
Because the entire anode assembly has to be contained within the evacuated tube shell 202, heat removal is a serious problem, further exacerbated by the higher power rating available. Direct cooling by conduction or convection, as in the Coolidge tube, is difficult. In most tubes, the anode 204 is suspended on ball bearings with silver powder lubrication, which provides almost negligible cooling by conduction.
The anode 204 must be constructed of high temperature materials. The focal spot temperature caused by electrons generated by cathode 208 impinging upon target 206 can reach 2500° C. during an exposure, and the anode assembly can reach 1000° C. following a series of large exposures. Typical materials used to form the anode are a tungsten-rhenium target 206 on a molybdenum core, backed with graphite. The rhenium makes the tungsten more ductile and resistant to wear from impact of the electron beams. The molybdenum conducts heat from the target. The graphite provides thermal storage for the anode, and minimizes the rotating mass of the anode.
Increasing demand for high-performance CT scanning and angiography systems has driven development of very high performance medical X-ray tubes. Contemporary CT tubes have power ratings of up to 100 kW and anode heat capacity of 6 Mj, yet retain an effective focal spot area of less than 1 mm2. Exemplary rotating anode X-ray tubes are shown in U.S. Pat. Nos. 1,192,706; 1,621,926; and 3,646,380, each of which is hereby incorporated by reference in its entirety.
In typical X-ray tubes, such as those described above, approximately 1% of the energy of the electron beam is converted to useful X-ray radiation, with 99% of the energy being lost as thermal energy. Thermal loss is of particular importance in high definition imaging, in which the electron beam must be focused on as small a target area as possible over a time period that is as short as possible. Image resolution depends upon both factors in diagnostic X-ray systems. Thermal energy gain within the target is a serious obstacle to the reduction of electron beam size or shortened exposure time.
Excess heat may be removed via conduction, as described above with reference to Coolidge tube 100, or the problem of instantaneous heating may be at least partially controlled by rotating the anode, as in rotating anode tube 200. Such solutions, however, only offer one degree of freedom in heat spreading. It would be desirable to provide an X-ray tube that can provide two degrees of freedom of heat dissipation, allowing for much higher instantaneous power limits.
Thus, an X-ray tube having a rotating and linearly translating anode solving the aforementioned problems is desired.
The X-ray tube having a rotating and linearly translating anode includes an evacuated shell having a substantially cylindrical anode rotatably mounted therein. The substantially cylindrical anode may be rotated through the use of any suitable rotational drive, and the substantially cylindrical anode is further selectively and controllably linearly translatable about the rotating longitudinal axis thereof. A cathode is mounted within the evacuated shell for producing an electron beam that impinges on an outer surface of the substantially cylindrical anode, thus forming a focal spot thereon. X-rays are generated from the focal spot and are transmitted through an X-ray permeable window formed in the evacuated shell.
These and other features of the present invention will become readily apparent upon further review of the following specification and drawings.
Similar reference characters denote corresponding features consistently throughout the attached drawings.
Now referring to
As shown, tube 10 includes a cathode 14 that emits an electron beam E. Electron beam E impinges upon anode 12 to form X-rays X. Anode 12 is mounted on a rotating shaft 16, as in the prior art rotating anode tube 200. As shown in
As best shown in
Returning to
As a further alternative, multiple bands of differing target materials may be formed on the surface of anode 12. In
It is to be understood that the present invention is not limited to the embodiments described above, but encompasses any and all embodiments within the scope of the following claims.
Number | Name | Date | Kind |
---|---|---|---|
1192706 | Thomson | Jul 1916 | A |
1211092 | Coolidge | Jan 1917 | A |
1621926 | Fujimoto | Mar 1927 | A |
1917099 | Coolidge | Jul 1933 | A |
1946312 | Coolidge | Feb 1934 | A |
2926270 | Zunick | Feb 1960 | A |
3398307 | Brown et al. | Aug 1968 | A |
3646380 | Hartl | Feb 1972 | A |
3836805 | Kok | Sep 1974 | A |
4300051 | Little | Nov 1981 | A |
4399551 | Grady | Aug 1983 | A |
4433431 | Pfeiler | Feb 1984 | A |
4658414 | Geldner | Apr 1987 | A |
4689809 | Sohval | Aug 1987 | A |
5305363 | Burke et al. | Apr 1994 | A |
6522721 | Lustberg | Feb 2003 | B1 |
6778633 | Loxley et al. | Aug 2004 | B1 |
7012989 | Holland et al. | Mar 2006 | B2 |
7248672 | Durst et al. | Jul 2007 | B2 |
7305063 | Heuscher | Dec 2007 | B2 |
7305066 | Ukita | Dec 2007 | B2 |
7315610 | Freudenberger et al. | Jan 2008 | B2 |
Number | Date | Country | |
---|---|---|---|
20100290594 A1 | Nov 2010 | US |