The present application is related generally to x-ray tubes.
An x-ray tube can make x-rays by sending electrons, across a voltage differential between a cathode and an anode, to a target of the anode. X-rays form as the electrons hit the target.
The following definitions, including plurals of the same, apply throughout this patent application.
As used herein, the terms “on”, “located on”, “located at”, and “located over” mean located directly on or located over with some other solid material between. The terms “located directly on”, “adjoin”, “adjoins”, and “adjoining” mean direct and immediate contact.
As used herein, the phrase “same material composition” means exactly the same, the same within normal manufacturing tolerances, or nearly exactly the same, such that any deviation from exactly the same would have negligible effect for ordinary use of the device.
As used herein, the term “tube” is not limited to a cylinder shape. The term “x-ray tube” is used because this is the normal term used for this x-ray device.
Unless explicitly noted otherwise herein, all temperature-dependent values are such values at 25° C.
As illustrated in
The enclosure, the cathode 11, and the anode 12 can define and form a housing that is hermetically sealed and capable of maintaining a vacuum therein. The enclosure can include a cylinder 15, disc(s) 62, or both. A hole can extend through a core of the cylinder 15. The term “cylinder” is used because this is a common shape; but the cylinder 15 can have other shapes. For example, the cylinder 15 can have a hollow conical frustum shape.
Transmission-target x-ray tubes 10, 20, 30, 40, 50, 90, and 100 are shown in the drawings, but the invention is equally applicable to reflection-target or side-window x-ray tubes.
The cathode 11 can include an electron-emitter 11EE (e.g. filament) for emitting electrons towards the anode 12. The anode 12 can include a target 14 (e.g. gold, rhodium, tungsten) for generation of x-rays. Electrons impinging on the target 14 can generate x-rays. The x-rays can emit out of the x-ray tube through an x-ray window 13.
Some electrons can rebound, and fail to form x-rays. These electrons can cause an electrical charge to build-up on an inner-face of the enclosure, such as on an inner-face 15i of the cylinder 15 and/or on an inner-face 62i of the disc(s) 62. The charge build-up can cause sharp voltage gradients within the enclosure, which can cause arcing failure of the x-ray tube. The inner-face of the enclosure can be the interior face of the enclosure facing inwardly towards a cavity of the x-ray tube.
The electrical charge can build unevenly on the inner-face of the enclosure. This uneven charge can shift the electron beam away from a center of the target 14. As a result of this shift, x-rays can emit from different locations of the target 14. Aiming a moving, or non-centered, x-ray beam can be difficult.
A triple-point is formed at a junction of (a) the enclosure, (b) an internal vacuum inside of the enclosure, and (c) the cathode 11 or anode 12. The triple-point can have high stress and large electric field gradients. Arcing failure of the x-ray tube can result from such high stress and large electric field gradients at the triple-point.
A coating-ring 18 and an interruption-ring 19 at the inner-face of the enclosure can reduce electrical charge build-up, avoid uneven electrical charge build-up, and can protect the triple-point. The coating-ring 18 and the interruption-ring 19 can be on the inner-face 15i of the cylinder 15, the inner-face 62i of the disc 62 of the cathode 11, the inner-face 62i of the disc 62 of the anode 12, or combinations thereof.
Part or all of the inner-face of the enclosure can be coated with an electrically resistive material, which can form a coating-ring 18. The coating-ring 18 can have a lower bulk electrical resistivity than the enclosure. The coating-ring 18 can provide a path for electrons on the inner-face of the enclosure to flow to ground. The coating-ring 18 can have surface resistivity (e.g. 1010-1014 Ohm per square) selected to allow only a small electrical current between cathode 11 and anode 12.
The coating-ring 18 can adjoin the cathode 11 or the anode 12. There can be multiple coating-rings 18, with one adjoining the cathode 11 and another adjoining the anode 12.
As illustrated in
The coating-ring 18 can encircle a longitudinal-axis 16 of the enclosure. The longitudinal-axis 16 can extend between and through the cathode 11 and the anode 12. The longitudinal-axis 16 can extend between and through the electron-emitter 11EE and the target 14. The longitudinal-axis 16 can be at a center of an electron beam and the cylinder 15.
An interruption-ring 19 at the inner-face of the enclosure can improve electric-field lines inside the enclosure. The interruption-ring 19 can provide a ring of higher electrical resistance per unit length, parallel to the longitudinal-axis 16, relative to the coating-ring 18. The interruption-ring 19 can pull electrical fields away from the triple-point, for protection of the triple-point. The interruption-ring 19 can be placed and sized for shaping of the electron-beam.
The interruption-ring 19 can be distinct from the coating-ring 18. The interruption-ring 19 can be structurally and dimensionally distinct or different from the coating-ring 18. For example, the interruption-ring 19 can have a different thickness and/or a different width than the coating-ring 18. The interruption ring 19 can be chemically distinct or different than the coating-ring 18. For example, the interruption ring 19 can comprise a different material than the coating-ring 18. The interruption-ring 19 can be located at a distinct or different location than the coating-ring 18. For example, the interruption ring 19 can be located at a different longitudinal and/or radial location than the coating ring 18.
The coating-ring 18 and the interruption-ring 19 can form a series electric-current-path 51 at the inner-face of the enclosure and between the anode 12 and the cathode 11, between the electron-emitter 11EE and the target 14, between the electron-emitter 11EE and the x-ray window 13, or combinations thereof. The electric-current-path 51 can extend longitudinally along a length of the cylinder 15 (see
The relatively higher electrical resistance per unit length of the interruption-ring 19 can help shape electrical field lines. Example resistance relationships, between the coating-ring 18 and the interruption-ring 19, include RC<RI, 2*RC<RI, 10*RC<RI, 100*RC<RI, 1000*RC<RI, 10,000*RC<RI. “RC” is electrical resistance per unit length through the coating-ring 18. “RI” is electrical resistance per unit length through the interruption-ring 19.
A smooth, linear, or gradual transition of electrical resistance per unit length, between RC and RI, can reduce sharp electrical field gradients. Electrical field gradients can also be reduced by multiple, small changes of electrical resistance per unit length, between RC and RI. As illustrated in
The coating-ring 18 can have a lower bulk electrical resistivity than the enclosure, thus providing a path of lower resistance for electrons on an interior of the enclosure to flow to ground. Thus. ρC<ρE, where ρC is bulk electrical resistivity of the coating-ring 18 and ρE is bulk electrical resistivity of the enclosure. The interruption-ring 19 can have bulk electrical resistivity that is higher than or equal to bulk electrical resistivity of the coating-ring 18. Thus, ρI≥ρC, where ρI is a bulk electrical resistivity of the interruption-ring 19. The interruption-ring 19 can have a bulk electrical resistivity that is lower than or equal to that of the enclosure (ρI≤ρE).
The coating-ring 18 and the interruption-ring 19 can be on the inner-face 15i of the cylinder 15, at an inner-face 62i of a disc 62 encircling at least part of the cathode 11, at an inner-face 62i of the disc 62 encircling at least part of the anode 12, or combinations thereof. The disc(s) 62 can be oriented perpendicular to the longitudinal axis 16. The cylinder 15 and/or the disc(s) 62 can be electrically insulative. The cylinder 15 and/or the disc(s) 62 can form the enclosure and can electrically insulate the cathode 11 from the anode 12.
The disc 62 can encircle a region 61. As illustrated in
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A choice between the number of interruption-rings 19 and the number of coating-rings 18, and whether they have a circular shape, a helical shape, or a spiral shape, can be made based on desired shaping of the electric-field lines and ease of manufacturing.
As illustrated in
As illustrated in
A choice between the designs of
A smooth, linear, or gradual transition change of material thickness between the thickness Th19 of the interruption-ring 19 and the thickness Th18 of the coating-ring 18 can reduce sharp electrical field gradients.
As illustrated in
The transition-region can have a smooth change of thickness Th17 from the thickness Th18 of the coating-ring 18 to the thickness Th19 of the interruption-ring 19 (Th19=0 in
The transition-region 17 can be applied to any other examples described herein.
The coating-ring 18 and the interruption-ring 19 can have the same material composition. For example, the interruption-ring 19 in
The coating-ring 18 and the interruption-ring 19 can have a different material composition with respect to each other. For example, the interruption-rings 19 in
A width WI of the interruption-ring 19 can be about 12% of a width WC of the cylinder 15 between the cathode 11 and the anode 12. For example, 0.01≤WI/WC, 0.05≤WI/WC, or 0.10≤WI/WC; and WI/WC≤0.15, WI/WC≤0.20, WI/WC≤0.40, WI/WC≤0.60, WI/WC≤0.90. WI is a width of the interruption-ring 19, and WC is a width of the cylinder 15 between the cathode 11 and the anode 12, each measured parallel to the longitudinal-axis 16 (see
Width WI, thickness Th19, location, and material of the interruption-ring 19 can be adjusted for desired resistivity to control high voltage fields and the flow of electrons along the inner-face of the enclosure.
A representation of half x-ray tubes 110 and 120, plus equipotential lines 123, are illustrated in
The equipotential lines 123 near the triple-point 121 of half x-ray tube 110 are closer to each other than those of half x-ray tube 120. Thus, the interruption-ring 19 of half x-ray tube 120 protects the triple-point 121 by spacing out equipotential lines 123 near the triple-point 121.
Equipotential lines 123 in half x-ray tube 120 converge due to the interruption-ring 19 at location 122. This convergence of equipotential lines 123 can be moved to different locations to shape or direct the electron beam. Thus, location, size, and resistance of the interruption-ring 19 is a tool for improving the design of the x-ray tube.
A method of making an enclosure to insulate a cathode 11 from an anode 12 in an x-ray tube, such as the enclosure described above, can comprise some or all of the following steps. The enclosure, the coating-ring 18, and the interruption-ring 19 can have properties as described above. The cylinder 15 is illustrated in
The method can comprise: (a) forming a coating-ring 18 and an interruption-ring 19 at an inner-face of the enclosure (see
The coating-ring 18 and the interruption-ring 19 can each encircle a longitudinal-axis 16 of the enclosure, such as the cylinder 15, at different locations along the longitudinal-axis 16 with respect to each other, as illustrated in
Forming the coating-ring 18 and the interruption-ring 19 can include masking a ring at the inner-face of the enclosure and coating an un-masked part of the inner-face. As illustrated in
Forming the coating-ring 18 and the interruption-ring 19 can include coating the inner-face of the enclosure, then removing part or all of a ring of the coating to form the interruption-ring 19. As illustrated in
If part of a thickness of a ring of the coating is removed by removal tool 141 to form the interruption-ring 19, then (a) the interruption-ring 19 can have bulk electrical resistivity equal to the coating-ring 18 (ρI=ρC); (b) the interruption-ring 19 can have higher electrical resistance per unit length than the coating-ring 18 (RI>RC); and/or (c) both the coating-ring 18 and the interruption-ring 19 have a bulk electrical resistivity that is less than that of the enclosure (ρI<ρE and ρC<ρE). See
If all of a ring of the coating is removed by removal tool 141 to form the interruption-ring 19, then the interruption-ring 19 can have (a) higher bulk electrical resistivity than the coating-ring 18 (ρI>ρC); (b) higher electrical resistance, per unit of length, than the coating-ring 18 (RI>RC); and/or (c) bulk electrical resistivity that is equal to that of the enclosure (ρI=ρE).
Forming the coating-ring 18 and the interruption-ring 19 can include depositing the coating on the inner-face with a tapered thickness. This could be done by masking, deposition time, or adjusting other coating distribution properties of the coating tool.
A spray tool 151, as shown in
This application is a continuation of U.S. patent application Ser. No. 17/500,403, filed on Oct. 13, 2021, which claims priority to U.S. Provisional Patent Application No. 63/112,216, filed on Nov. 11, 2020, which are incorporated herein by reference.
Number | Date | Country | |
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63112216 | Nov 2020 | US |
Number | Date | Country | |
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Parent | 17500403 | Oct 2021 | US |
Child | 18311683 | US |