Classifications

• • H—ELECTRICITY
  • H01—ELECTRIC ELEMENTS
  • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
  • H01J35/00—X-ray tubes
  • H01J35/02—Details
  • H01J35/16—Vessels; Containers; Shields associated therewith
• • H—ELECTRICITY
  • H01—ELECTRIC ELEMENTS
  • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
  • H01J35/00—X-ray tubes
  • H01J35/02—Details
  • H01J35/04—Electrodes ; Mutual position thereof; Constructional adaptations therefor
  • H01J35/06—Cathodes
  • H01J35/064—Details of the emitter, e.g. material or structure
• • H—ELECTRICITY
  • H01—ELECTRIC ELEMENTS
  • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
  • H01J35/00—X-ray tubes
  • H01J35/02—Details
  • H01J35/04—Electrodes ; Mutual position thereof; Constructional adaptations therefor
  • H01J35/06—Cathodes
  • H01J35/066—Details of electron optical components, e.g. cathode cups
• • H—ELECTRICITY
  • H01—ELECTRIC ELEMENTS
  • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
  • H01J35/00—X-ray tubes
  • H01J35/02—Details
  • H01J35/14—Arrangements for concentrating, focusing, or directing the cathode ray
  • H01J35/147—Spot size control
• • H—ELECTRICITY
  • H01—ELECTRIC ELEMENTS
  • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
  • H01J2235/00—X-ray tubes
  • H01J2235/06—Cathode assembly
  • H01J2235/068—Multi-cathode assembly
• • H—ELECTRICITY
  • H01—ELECTRIC ELEMENTS
  • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
  • H01J2235/00—X-ray tubes
  • H01J2235/12—Cooling
  • H01J2235/1225—Cooling characterised by method
  • H01J2235/1262—Circulating fluids
  • H01J2235/1287—Heat pipes

Definitions

• the present invention relates generally to X-ray tube technology. More specifically, this invention pertains to a new configuration for a low power X-ray source for an X-ray fluorescence instrument having an air-cooled and metal-ceramic design which provides for a higher flux of X-rays as compared with X-ray tubes of similar power input. Most advantageously, the configuration of the cathode assembly and the anode assembly is such that a small nose at the end- window is provided, thereby enabling the X-ray source to be close to a sample being irradiated.
• a cathode assembly and an anode assembly are vacuum sealed in a glass envelope. Electrons are generated by at least one cathode filament in the cathode assembly. These electrons are accelerated toward the anode assembly by a high voltage electrical field. The high energy electrons generate X-rays upon impact with the anode assembly. An unavoidable by-product of this process is the generation of substantial amounts of heat. It is important to the life of the X-ray tube to dissipate the heat as efficiently as possible.
• the X-ray tube described above is mounted within a housing for protecting the surrounding environment from unwanted X-rays.
• a state of the art method for cooling the X- ray tube is to fill the housing with oil.
• the oil not only provides electrical insulation, but it also absorbs the heat generated by the anode assembly.
• the requirement of an oil pump and hoses also results in lower system reliability, the possibility of leaks and fire, as well as extra cost. Oil cooling also makes repair and maintenance of the X-ray tube more difficult.
• X-ray tube utilized in X-ray fluorescence (XRF)
• XRF X-ray fluorescence
• the X- ray source be as close as possible to a subject or sample being irradiated.
• the result of X-rays being absorbed by the sample is that it fluoresces.
• a detector of fluorescent energy is then disposed near to the sample at a desired angle relative to the sample and the X-ray source. The desired angle typically enables the maximum amount of fluorescent energy to be received by the fluorescent energy detector.
• X-ray tubes which are utilized in X-ray fluorescence instruments are typically characterized as being one of three different X-ray tube configurations. These X-ray tube configurations are known as a transmission tube design having an end-window from which X- ray energy is directed toward a sample, and a side-window configuration.
• FIG 1 shows that a housing 12 surrounds a cathode assembly 14.
• the cathode assembly 14 is centered behind an anode/window combination 16.
• a high voltage field developed between the cathode assembly 14 and the anode/window 16 causes electrons 18 emitted from a filament (not shown) in the cathode assembly 14 to flow directly toward the anode/window 16.
• the anode/window 16 can be coated with an anode-type material.
• the electron flux 18 striking the anode/window 16 causes the generation of X-rays 20.
• the usable X-rays 21 continue out through the anode/window 16. Accordingly, instead of electrons 18 striking an anode and the resulting X-rays 20 being deflected therefrom at an angle, the usable X-rays 21 continue on in the same direction as the original flow of electrons 18 from the cathode assembly 14.
• the high voltage stability of a transmission tube is generally not as good as from a side-window X- ray tube design.
• the anode/window is also constructed differently because of the substantial amount of heat which is generated. This heat imposes a limit on how thin the anode/window can be constructed.
• the X-rays produced on the surface of the anode are substantially attenuated on passing through the entire thickness of the anode window. Consequently, the X-ray emissions are not as strong as they could be.
• the end- window tube design has inherent design drawbacks which prevent it from being more useful in an X-ray fluorescence detector. Specifically, the size of the X-ray tube nose interferes with optimum detector placement.
• the side-window X-ray tube also has serious drawbacks which typically prohibit or hinder its application in XRF instruments.
• drawbacks stem from the fact that the sample-to-target distance is necessarily large. The distance is large because as shown in the cross section view of an X-ray tube 22 provided in figure 2, the X-ray tube itself interferes with the detection of fluorescent energy 24 because a fluorescent energy detector 26 can not be placed in optimal locations. In other words, the sidewall 28 of the X-ray tube 22 absorbs much of the fluorescent energy 24 which would otherwise be detected at the optimal detection angle.
• moving the side- window X-ray tube further from the sample simply decreases the available X-ray flux at the sample. The available X-ray flux is already inherently small due to the large distance from the target 31 to the sample 30 in the side- window tube.
• the present invention is realized in an X-ray tube device and a method for construction thereof which places the cathode assembly and the anode assembly in a nose of the X-ray tube, wherein an emitter face of each assembly is directed toward an X-ray emission end thereof.
• the electrons emitted from the cathode assembly travel along a path outward until striking the anode assembly which then generates the X-rays which are directed toward a beryllium window in the X-ray tube.
• This advantageous structure enables the target anode-to- window distance to be small, resulting in a large X-ray flux towards a sample.
• the small nose of the X- ray tube enables a fluorescence detector to be positioned in an optimal location because the X- ray tube's shape does not displace the fluorescence detector.
• the window is operated at cathode potential so that no electrons strike and thus heat the window.
• a potting material utilized in the construction which is normally a poor thermal conductor, is modified so as to provide improved thermal conduction.
• Enhanced cooling of the X-ray tube is then accomplished by cooling an exterior surface of the potting material, such as through forced-air.
• projections or protrusions are formed on the exterior surface of the potting material. Forced-air cooling is thus more effective because of the increased surface area of the potting material which can be cooled.
• the use of oil as a high voltage insulator and cooling mechanism is replaced with the air-cooled system. Accordingly, the complexity of the overall system and the cost is decreased while reliability is increased.
• the high voltage insulation is increased in length and the diametric spacing between components is increased, advantageously resulting in higher voltage operation of the X-ray tube.
• a second cathode assembly is provided which is separate from the first cathode assembly, thereby providing for dual focal spot capability.
• the filaments could be operated simultaneously for higher X-ray flux emissions.
• an electrode grid can be provided for 1) enhanced control of a focal spot location, 2) enhanced electron emission from the cathode assembly, or achieving control over a size of a focal spot which is other wise unobtainable using a basic electron optic configuration.
• a heat pipe is provided inside the anode assembly to thereby permit higher power operation.
• the heat pipe makes possible the use of alternate target materials having higher vapor pressures which therefore require enhanced cooling for practical use.
• an electrically flashed getter is provided for improved removal of gas molecules from the vacuum envelope of the X-ray tube, thus resulting in a X-ray tube which is cleaner.
• a cathode slot design having a coiled filament is borrowed from medical application X-ray tube designs to provide more efficient electron emission and improved focal spot size repeatability.
• Figure 1 is a cross-sectional profile view of some of the typical components in an X-ray tube of the prior art, where the design is known as a transmission tube wherein an anode is constructed as part of an X-ray emission end-window.
• Figure 2 is a cross-sectional end view of a side-window X-ray tube which is also typical of the prior art, and by the very nature of its construction interferes with the detection of energy emitted from a fluorescing sample under observation.
• Figure 3 is a cross-sectional profile view of a presently preferred embodiment made in accordance with the specifications of the present invention.
• Figure 4 is a close-up cross-sectional view of the X-ray tube of figure 3.
• Figure 5 is a profile of electron beam flux lines which are being emitted from the cathode filament. The electron beam flux lines then strike the anode assembly on the X-ray emission face.
• Figure 6 is provided to show an end-view of a cathode head relative to a focusing electrode.
• Figure 7 is an orthogonal view of the cathode head which more readily portrays the angle of the cathode electron emission face, the two lead holes and the focusing slot.
• Figure 8 is an orthogonal view of the focusing electrode which shows the U-shape of the preferred embodiment.
• Figure 9 is a first alternative embodiment showing the projections which are formed of the potting material which has been modified so as to have greater thermal conductivity.
• the present invention encompasses many improvements in the design of X-ray tubes.
• the presently preferred embodiment of the present invention has particular application to X-ray tubes which are utilized in X-ray fluorescence instruments. This is because one of the important points of novelty of the preferred embodiment is an advantageous arrangement of a cathode assembly and an anode assembly within the X-ray tube.
• Figure 3 shows that the presently preferred embodiment is an X-ray tube 30 which has an end- window configuration. That is to say, an X-ray emission window 32 is disposed at one end of the X-ray tube 30.
• Housed within a vacuum envelope 34 are a cathode assembly 36 and an anode assembly 38.
• the vacuum envelope 34 is partially enclosed by a high voltage insulator 40.
• the high voltage insulator 40 is in turn surrounded by a potting material 42.
• electrical leads such as the anode lead 44, and at least two filament leads 45a and 45b which deliver voltages to the anode assembly 38 and the cathode assembly 36, respectively.
• An o-ring groove 58 is also shown to circumscribe the X-ray tube 30. The o-ring 58 is for providing a seal when the sample 52 is being irradiated within a vacuum chamber (not shown).
• the cathode assembly 36 is shown having a very different orientation relative to the anode assembly 38 than is taught in the prior art. Instead of an electron emission face 46 of the cathode assembly 36 being orientated towards an X-ray emission face 48 of the anode assembly 38, both emission faces 46 and 48 are directed toward the X-ray emission window 32.
• the nose of this X-ray tube 30 is defined generally by the dotted line 50. Specifically, it is that portion of the X-ray tube 30 which is closest to a sample 52 being irradiated and which can interfere with or block energy being radiated from the sample. In other words, information is derived from an irradiated sample 52 by monitoring and detecting energy which is fluorescing therefrom. Accordingly, at least one energy detector 54 is disposed near the sample 52 as shown.
• one optimal angle for energy detection is at approximately a forty five degree angle relative to an X-ray tube axis 56. Therefore, with the at least one energy detector 54 positioned as shown in figure 3, the appropriate angle is obtained. While this explanation shows the end result of the preferred embodiment, some important aspects of implementation are worth examination.
• Figure 4 is a close-up cross-sectional view of the X-ray tube 30 of figure 3. This view is helpful in that additional components are easier to identify. Specifically, in addition to the cathode and anode assemblies 36 and 38, there is a shown a focusing electrode 60, an end-view of a cathode filament 62, and a filament lead 76 which provides an electrical contact to the filament.
• the design of the cathode assembly 36 is based on a cathode assembly utilized in medical applications, such as in X-ray tubes used in mammography applications.
• Mammography cathode assemblies are characterized as having a focusing slot 64 as shown.
• the focusing slot 64 is designed to focus a width of an electron beam being generated by the cathode filament 62.
• multi-level slots also referred to as cathode cups
• the advantages of leaving the cathode filament 62 out of the slot 64 are very desirable.
• the perveance obtained by leaving the cathode filament 62 out of the slot 64 is considerably larger than with mammography tubes. In one such embodiment, a 10mA emission current at 4kV X-ray tube voltage is achievable at a practical filament temperature.
• the cathode filament 62 might be able to supply a desired level of electron emissions at a substantially smaller voltage level. Accordingly, the cathode filament 62 can run at a lower temperature. Therefore, the cathode filament 62 lasts longer because there is less evaporation of tungsten, or of whatever material is being used as the cathode filament 62.
• cathode filament 62 in a cathode assembly 36 is much easier than in other cathode assemblies. Furthermore, the cathode filament 62 can be placed much more precisely to obtain more predictable results, even when utilizing a number of different X-ray tubes 30.
• Figure 5 is a profile of electron beam flux lines 70 which are being emitted from the cathode filament 62.
• the electron beam flux lines 70 then strike the anode assembly 38 on the X-ray emission face 48.
• the number of flux lines shown is only relevant in that the curved path of the electrons is being illustrated from all relevant angles around the cathode filament 62.
• the path that the electron beam flux lines 70 must travel is purely a function of the location of the emission faces 46 and 48, and window 32. Nevertheless, it should be realized that to take advantage of the preferred embodiment, the orientation of the cathode assembly 36 and the anode assembly 38 will be such that the electron beam flux lines 70 are going to be curving back toward the X-ray emission face 48. Accordingly, it should be apparent that the cathode assembly is preferably (but not exclusively) going to have its electron emission face directed toward the X-ray emission window 32.
• the cathode assembly is going to be at an angle so that it is providing a smaller nose 50, it is always going to be angled so that the electron beam flux lines 70 must travel along a path which bends at least forty five degrees relative to the X-ray tube axis 56.
• the cathode 62 filament is disposed partially down into the slot 64. As explained above, while this is certainly allowable, a substantially greater perveance is obtained by lifting the cathode filament 62 generally above a plane formed by the cathode electron emission face 46. Note that this figure does not show the cathode filament 62 raised above the plane of the electron emission face 46.
• Figure 6 is provided to show an end-view of a cathode head 72.
• the cathode head 72 shows from this angle that there are two holes 74 (seen on their ends) through the cathode head 72.
• a lead 76 In the center of each hole 74 is a lead 76, where the cathode filament 62 is generally disposed therebetween.
• the focusing electrode 60 Also shown in this end-view is the focusing electrode 60.
• the distinctive U-shape design of this preferred focusing electrode 60 enables it to bend around the anode assembly 38.
• the ends 82 of the U-shape terminate just short of physical contact with the cathode 72.
• figure 7 is also provided.
• Figure 8 is provided to also assist in visualizing the focusing electrode 60.
• Figure 8 is an orthogonal view of the focusing electrode 60 which shows the U-shape of the preferred embodiment. It should be remembered that a focusing electrode can have any desired shape which accomplishes the type of focusing (length, width, or other) which is desired.
• the present invention is also directed to a low power application, on the order of 50 watts or less.
• This low power provides the opportunity to substitute a simpler cooling method for the oil or SF6 used in the prior art.
• Forced-air cooling can be particularly advantageous because of cost, weight, materials, etc.
• an alternative embodiment of the present invention adapts the X-ray tube to more readily take advantage of air cooling.
• the potting material of the present invention is modified by the addition of a second material. A powder comprised of boron nitride power is added to a typical silicone potting material.
• FIG. 9 shows a plurality of projections which are formed from the potting material and on the exterior surface thereof.
• Figure 9 shows that the projections 78 are preferably cylindrical in shape. This is very simple to put into practice. However, it should be readily apparent that any shape for the projections 78 can be used.
• a preferred embodiment has three rows often projections 78 each.
• the projections 78 can also be arranged differently, such as in a staggered pattern, with or without regular spacing.
• the presently preferred embodiment teaches that the anode assembly 38 is co-linear and co-axial with the X-ray tube axis 56.
• the anode assembly 38 might be co-linear but not co-axial and generate an X-ray beam which is offcenter from the X-ray tube axis 56.
• the anode assembly 38 might not be coaxial or co-linear.
• more than one cathode assembly 36 be provided in the X-ray tube.
• a diametrically opposite second cathode assembly might be disposed in the vacuum chamber. This would allow for two options to occur. First, the cathode assemblies could be operated at different times, where each cathode assembly has its own focal spot characteristics of size, length, width, etc. Second, the cathode assemblies could be operated simultaneously so as to act to reinforce each other. This could double X-ray emissions, but would require a greater ability to cool the X-ray tube cathode structure. It is possible to couple a heat pipe to the anode assembly. The heat pipe might also be utilized when it is desirable to utilize different materials for the anode assembly.
• an electrical grid can be placed over the electron emission face 46.
• the electrical grid can have an electrical charge applied thereto, resulting in a modification of the focal spot.
• This electrical grid can be an alternative means of focal spot characteristics.
• the present invention incorporates an electrically flashed getter.
• the getter is able to significantly improve the cleanliness of the vacuum chamber within the X-ray tube, thereby enabling improved performance over the life of the X-ray tube.

Landscapes

• X-Ray Techniques (AREA)

Priority Applications (4)

Applications Claiming Priority (2)

Publications (1)

Family

ID=25446039

Family Applications (1)

Country Status (6)

Cited By (2)

Families Citing this family (55)

Citations (4)

Family Cites Families (1)

• 1997
  • 1997-09-02 US US08/921,830 patent/US6075839A/en not_active Expired - Lifetime
• 1998
  • 1998-09-01 DE DE69839550T patent/DE69839550D1/de not_active Expired - Fee Related
  • 1998-09-01 WO PCT/US1998/018147 patent/WO1999012182A1/en not_active Ceased
  • 1998-09-01 JP JP51696099A patent/JP4308332B2/ja not_active Expired - Lifetime
  • 1998-09-01 EP EP98943509A patent/EP0935811B1/en not_active Expired - Lifetime
  • 1998-09-01 CA CA002268137A patent/CA2268137A1/en not_active Abandoned

Patent Citations (4)

Also Published As

Similar Documents

Legal Events