Apparatus and method for rapidly switching the energy spectrum of diagnostic X-ray beams

Information

  • Patent Application
  • 20080063145
  • Publication Number
    20080063145
  • Date Filed
    September 12, 2006
    17 years ago
  • Date Published
    March 13, 2008
    16 years ago
Abstract
An X-ray imaging apparatus is disclosed. The apparatus includes a radiator housing, an X-ray tube, a source of X-rays and at least one filtration material disposed on the X-ray tube. The X-ray tube is rotatable about a longitudinal axis and is disposed at least partially within the radiator housing. The source of X-rays emits at least one X-ray beam at least partially through the X-ray tube. The X-ray beam exits the X-ray tube at an annular X-ray window. The filtration material at least partially covers a portion of the annular X-ray window. Rotation of the X-ray tube causes the X-ray beam to pass through a plurality of locations in the annular X-ray window and at least a portion of the X-ray beam is filtered by the filtration material.
Description

BRIEF DESCRIPTION OF THE DRAWINGS

The disclosure will become more clearly understood from the following detailed description in connection with the accompanying drawings, in which:



FIG. 1 is side sectional view of an X-ray imaging apparatus including a rotating bulb tube having a filtration material thereon according to an embodiment of the present disclosure;



FIG. 2 is a perspective view of the rotating bulb tube of FIG. 1; and



FIGS. 3A-3F illustrate cross sectional views of the rotating bulb tube of FIGS. 1 and 2 having filters variously oriented thereon.





DETAILED DESCRIPTION

The following description is presented to enable one of ordinary skill in the art to make and use the disclosure and is provided in the context of a patent application and its requirements. Various modifications to the disclosed embodiments will be readily apparent to those skilled in the art and the generic principles herein may be applied to other embodiments. Thus, the present disclosure is not intended to be limited to the embodiment shown but is to be accorded the broadest scope consistent with the principles and features described herein.


Referring now to the drawings, and initially to FIG. 1, an X-ray apparatus, for example an X-ray tomography apparatus, in accordance with the present disclosure is shown and is generally referenced by numeral 100. In the illustrated embodiment, X-ray tomography apparatus 100 includes a radiator housing 110 and an X-ray tube 120 disposed therein. X-ray tube 120 includes a first portion 122 and a second portion 124 and is rotatable about longitudinal axis A-A extending therethrough. Here, X-ray tube 120 includes a vacuum housing 130 with a rotating anode 140 rigidly connected thereto. This embodiment also includes shaft stubs 150, 160 attached to vacuum housing 130 and to rotating anode 140, respectively. Further, X-ray tube 120 may include a voltage setting in the range of about 40 kilovolts to about 160 kilovolts. Additionally, X-ray tube 120 is illustrated seated in two bearings 170 and 180 and is in mechanical cooperation with a motor 190 and coupling 200 to facilitate rotation.


In the illustrated embodiment, the entire interior of radiator housing 110, except for the space accepting motor 190 and sealed by a suitable seal 210 and is filled with a fluid coolant 221, such as an electrically insulating oil.


As illustrated in FIG. 1, a source of electrons 220, such as a cathode, generates an electron beam 230. In an embodiment, a Wehnelt electrode 240 focuses electron beam 230. Here, electron beam 230 is deflected by an electromagnetic deflection system 250 enabling electron beam 230 to strike rotating anode 140, which rotates with X-ray tube 120, in a stationary point, namely a focal spot 260. X-ray beams 270 then emanate from focal spot 260 (e.g., source of X-ray beams 270). Only a central beam is illustrated in FIG. 1 for clarity. X-ray beams 270 emerge from X-ray tube 120 through vacuum housing 130 and exits radiator housing 110 through an annular X-ray window 280. Although not explicitly illustrated, the use of multiple focal spots is envisioned by this disclosure.


In use, X-ray tube 120 rotates along its longitudinal axis A-A. X-ray beams 270 are emitted through X-ray tube 120 and exits X-ray tube 120 through annular X-ray window 280. Annular X-ray window 280 is disposed around the periphery of X-ray tube 120 and allows X-ray beams 270 to pass therethrough.


According to an embodiment of the present disclosure, at least one filtration material 300 is disposed on X-ray tube 120. Filtration material 300 at least partially covers a portion of annular X-ray window 280, thus filtering X-ray beams 270 as they pass therethrough. As illustrated in FIGS. 1-3, filtration material 300 is disposed in a plurality of spaced-apart locations on X-ray tube 120 and around its periphery. As illustrated in FIGS. 3A, 3C and 3E a first filtration material 300a is disposed on X-ray tube 120. Here, rotation of X-ray tube 120 causes X-ray beams 270 to be intermittently filtered by first filtration material 300a as it passes through X-ray tube 120. It shall be noted that in such an embodiment, the material of X-ray tube 120 (and/or annular X-ray window 280) may also act as a filter.


As shown in FIGS. 1, 2, 3B, 3D and 3F, a first filtration material 300a and a second filtration material 300b are included. Here, the filtration materials 300a, 300b (see FIG. 2) are an alternating orientation and are at least partially covering annular X-ray window 280. In such embodiments, as X-ray tube 120 rotates, X-ray beams 270 are filtered in an alternating fashion, thus rapidly switching the energy spectrum of X-ray beams 270. Such an embodiment may facilitate providing dual-energy imaging, which may be helpful, for example, in enhancing the ability to distinguish bone from contrast.


It is envisioned that first filtration material 300a strongly absorbs X-ray beams 270 whose energy is in the lower half of the spectrum, which extends from 0 to the tube's operating kVp. Second filtration material 300b absorbs the lower part of the spectrum more weakly, while reducing the combined X-ray intensity to approximately the intensity level provided by first filtration material 300a.


It is envisioned that first filtration material 300a is made from a material whose K-Shell electron binding energy is outside the range of about 30 keV to about 120 keV, such as aluminum. It is further envisioned that second filtration material 300b is made from a material whose binding energy is within the range of about 30 keV to about 120 keV, such as an actinide, including uranium or thorium.


With reference to FIGS. 3A-3F, X-ray tube 120 includes an exterior surface 126 and an interior surface 128. Filtration material 300 may be disposed on exterior surface 126 (FIGS. 3A, 3B and 3E), interior surface 128 (FIGS. 3C and 3D), or a combination of exterior surface 126 and interior surface 128 (FIG. 3F) of X-ray tube 120.


In an embodiment of the disclosure, filtration material 300 may be made of at least one material including aluminum, thorium, uranium, titanium, gold, lead, tungsten, tin, copper, iron, for example. Filtration material 300 may also be made of at least one rare-earth material including, for example, erbium, samarium or neodymium.


With reference to FIGS. 3A-3F, it is also envisioned that the thicknesses of filtration materials 300 may not be constant across their length and/or width (the thicknesses of the materials in FIGS. 3A-3F are not to scale). The thickness may be based on the material being used as filtration material 300 and on the amount of filtration desired. For example, it is contemplated that the thickness of first filtration material 300a is in the range of about 5 mm to about 7 mm, in the case of aluminum, and possibly equal to about 6 mm. Additionally, it is contemplated that the thickness of second filtration material 300b is in the range of about 40 μm to about 60 μm, in the case of uranium or thorium, and possibly equal about 50 μm. Further, as indicated by FIGS. 3E and 3F, the thickness of first filtration material 300a and/or second filtration material 300b may vary around the circumference of the tube.


It is envisioned that filtration materials 300 are removably attached to X-ray tube 120 to enable use for dual-energy imaging (when filtration materials 300 are attached to X-ray tube 120) and for normal operation (when filtration materials 300 are removed from X-ray tube 120).


The present disclosure also relates to a method for rapidly switching the energy spectrum of X-ray beams 270, for example, diagnostic X-ray beams. The method includes providing an X-ray tomography apparatus 100, such as that described above. The method further includes rotating X-ray tube 120 to cause X-ray beams 270 to pass through a plurality of locations in annular X-ray window 280.


Other applications for use of the X-ray apparatus 100 include various X-ray imaging devices. Such devices include CT scanners (including medical CT scanners) and medical X-ray imaging devices (also including medical CT scanners). Additionally, an embodiment of the apparatus and/or method disclosed in the present application may be used in angiography and in conjunction with baggage screening machines (e.g., in airports).


Although the present disclosure has been described in accordance with the embodiments shown, one of ordinary skill in the art will readily recognize that there could be variations to the embodiment and these variations would be within the spirit and scope of the present disclosure. Accordingly, many modifications may be made by one of ordinary skill in the art without departing from the spirit and scope of the appended claims.

Claims
  • 1. An X-ray imaging apparatus, comprising: a radiator housing;an X-ray tube being rotatable about a longitudinal axis defined therethrough and being disposed at least partially within the radiator housing, the X-ray tube including a first portion and a second portion;a source of X-ray beams which emits at least one X-ray beam at least partially through the X-ray tube and exiting the X-ray tube at an annular X-ray window peripherally disposed on the X-ray tube adjacent the second portion;at least one filtration material disposed on the X-ray tube and at least partially covering a portion of the annular X-ray window, wherein the X-ray beam becomes filtered as it passes through the filtration material; andwherein rotation of the X-ray tube causes the X-ray beam to pass through a plurality of locations in the annular X-ray window and wherein at least a portion of the X-ray beam is filtered by the filtration material.
  • 2. The X-ray imaging apparatus of claim 1, wherein the at least one filtration material is disposed in a plurality of spaced-apart locations on the X-ray tube.
  • 3. The X-ray imaging apparatus of claim 1, wherein the X-ray tube includes an interior surface and an exterior surface and wherein the at least one filtration material is disposed on an interior surface of the X-ray tube.
  • 4. The X-ray imaging apparatus of claim 1, wherein the X-ray tube includes an interior surface and an exterior surface and wherein the at least one filtration material is disposed on an exterior surface of the X-ray tube.
  • 5. The X-ray imaging apparatus of claim 1, wherein the at least one filtration material is essentially comprised of uranium.
  • 6. The X-ray imaging apparatus of claim 1, wherein the at least one filtration material is essentially comprised of thorium.
  • 7. The X-ray imaging apparatus of claim 1, wherein the X-ray imaging apparatus includes a first filtration material and a second filtration material, a plurality of the first filtration material and a plurality of the second filtration material being disposed in an alternating orientation at least partially covering the annular X-ray window.
  • 8. The X-ray imaging apparatus of claim 7, wherein the first filtration material is made from a material whose K-Shell electron binding energy is outside the range of about 30 keV to about 120 keV and the second filtration material is made from a material whose K-Shell electron binding energy is within the range of about 30 keV to about 120 keV.
  • 9. The X-ray imaging apparatus of claim 7, wherein the first filtration material is aluminum and the thickness is in the range of about 5 mm to about 7 mm.
  • 10. The X-ray imaging apparatus of claim 9, wherein the second filtration material is uranium and the thickness is in the range of about 40 μm to about 60 μm.
  • 11. The X-ray imaging apparatus of claim 1, wherein the X-ray tube includes a voltage setting in the range of about 40 kilovolts and 160 kilovolts.
  • 12. The X-ray imaging apparatus of claim 1, wherein the radiator housing is at least partially filled with a coolant.
  • 13. The X-ray imaging apparatus of claim 1 further defined as an X-ray Computed Tomography (CT) apparatus.
  • 14. A method for rapidly switching the energy spectrum of X-ray beams, comprising: providing an X-ray imaging apparatus, including: a radiator housing;an X-ray tube being rotatable about a longitudinal axis defined therethrough and being disposed at least partially within the radiator housing;a source of X-ray beams which emits at least one X-ray beam at least partially through the X-ray tube and exiting the X-ray tube at an annular X-ray window peripherally disposed on the X-ray tube; andat least one filtration material disposed on the X-ray tube and at least partially covering a portion of the annular X-ray window; androtating the X-ray tube to cause the X-ray beam to pass through a plurality of locations in the annular X-ray window.
  • 15. The method of claim 14, wherein the X-ray imaging apparatus includes a first filtration material and a second filtration material, a plurality of the first filtration material and a plurality of the second filtration material being disposed in an alternating orientation at least partially covering the annular X-ray window.
  • 16. The method of claim 15, wherein the first filtration material is made from a material whose electron binding energy is outside the range of about 30 keV to about 120 keV and the second filtration material is made from a material whose electron binding energy is within the range of about 30 keV to about 120 keV.
  • 17. The method of claim 14, wherein the at least one filtration material is essentially comprised of an actinide.
  • 18. (canceled)
  • 19. (canceled)
  • 20. (canceled)