X-Ray Tube

The invention relates to an x-ray tube according to the preamble of patent claim 1. X-ray tubes of this type are, for example, known from the publication (page 15) "Concerning The History of Medical X-Ray Tubes" by F. Prellwitz, Medical Technology Department of the Siemens Aktiengesellschaft, Erlangen, Germany, Order No. MR 71/1524, printed in the Federal Republic of Germany SD 06792.5.

In the case of the known tube, the tube housing and the shielding were at the same potential, so that a disruptive discharge through the glass tube envelope was largely prevented. However, an electrode interposed between the focus and the x-ray shield led to an impairment of the attainable X-ray beam. Further, it was disadvantageous here that a difficult and expensive glass technology was necessary, on the one hand, and that, given high tube performances and tube powers conventional today, the shielding, necessarily thermally largely insulated in the case of this method of construction, becomes impermissibly highly heated.

It is the object of the invention, in the case of an X-ray tube according to the preamble of patent claim 1, in addition to providing an improvement in the dielectric strength and a manufacturing-sympathetic construction, to render possible close-to-focus beam delineation and to obtain an increased anode load carrying capacity. In accordance with the invention, this object is achieved by the measures disclosed in the characterizing clause of claim 1. Advantageous further developments and designs of the invention are the subject of the sub-claims.

Through the utilization of a shield, which is connected to a potential which is greater than half the tube voltage but smaller than the anode potential, in solving the above problem, the result is that a greater portion--in relation to known tubes--of the backscatter electrons is withdrawn from the focal spot, as a consequence of which the anode load carrying capacity increases. Moreover, the fraction of outside-of-focus radiation in the active X-ray beam is decreased. Furthermore, a very close-to-focus delineation or collimation of the cone of rays is possible, because the potential difference between the shield and the anode is less and therefore the distance between the focus and the beam delineating window in the shield can be smaller than in the case of hitherto employed arrangements.

In an advantageous fashion, the inventive shield can be support-mounted on a metal ring which is disposed concentrically to the discharge space. The metal ring can bear, at its one end, an insulating part to which the cathode is mounted, and, at its other end, it can bear an insulating part which bears the anode. In utilizing known advantageous technologies, the insulating parts can consist of glass, so that the conventional glass blowing technique can be employed.

As a rule, the shield receives the shape of a cylinder which encloses the cathode as well as the anode. The thereby resulting, largely metallically limited discharge space prevents the glass wall of the tube envelope from being struck by electrons and metal vapor-depositions. Moreover, long insulation distances remain which guarantee great dielectric strength.

Further details and advantages of the invention shall be explained on the basis of the exemplary embodiment illustrated on the accompanying drawing sheet; and other objects, features and advantages will be apparent from this detailed disclosure and from the appended claims.

The single FIGURE is a somewhat diagrammatic longitudinal sectional view showing a rotary anode x-ray tube constructed in accordance with the present invention.

In the exemplary embodiment of the rotary anode X-ray tube 1, illustrated in section 2, designates a metal ring consisting of Vacon which has the shape of an approximately fifteen millimeter (15 mm) long tube piece whose wall is one millimenter (1 mm) thick and which is connected at its one end with a glass part 3 on the interior side of which a cathode arrangement 4 is supported. At its other end, the metal ring 2 bears a glass part 5 which exhibits an anode arrangement 6 at its end. The anode arrangement is comprised of an anode plate 7, a supporting shaft 8, and a rotor 9 for driving shaft 8. A support tube 10 supports rotor 9 and is fixedly mounted on the glass part 5. On the interior side of the ring 2, a shield 11 is mounted which is fixed in the tube 1 via retaining connections 12. As the shield, in the present example, a copper (Cu) plate is employed which is 1.5 mm thick. Also other metal plates, such as e.g. those consisting of nickel or high-grade steel, are suitable for the shield 11 if they are stable given the conditions in the tube.

In order to generate X-rays a filament current is applied between lines 20 and 21 in a manner known per se, which filament current brings the cathode 22 to incandescence. Moreover, via one of the lines 20 and 21 as well as a conductor within support tube 10 connecting with shaft 8, the tube voltage is applied to the tube, so that an electron flow 23 impacts on a focal spot path 24 of the anode plate 7. An X-ray cone 25 is thereby generated which emerges toward the exterior through a window 26 in the shield 11 and the window 27 in the tube envelope. The two windows 26 and 27, in an advantageous manner, consist of beryllium and represent 0.5 mm-thick sheets which are inserted in corresponding openings of the shield 11 and in the wall 5 of the glass tube part, respectively.

It will be apparent that many modifications and variations may be effected without departing from the scope of the novel concepts and teachings of the present invention.

Referring to the drawing, a conductor 28 is diagrammatically indicated for supplying anode potential U.sub.A to the anode plate 7 via the shaft 8. The cathode conductor 20, for example may be at ground potential (zero volts). For supplying the shield potential U.sub.S as explained herein, a conductor 29 is connected with the shield 11. The potential supplied to the shield 11 may have a value U.sub.S greater than one-half of anode potential, U.sub.A, but less than total anode potential; that is U.sub.A >U.sub.S >U.sub.A/2. For purposes of diagrammatic illustration, conductor 29 is indicated as being electrically connected with the shield 11 via metal ring 2 and metallic retaining connections 12.

In the drawing the shield 11 is shown as comprising a generally cylindrical portion surrounding the anode 7 and cathode 22 and providing x-ray shielding except at the x-ray permeable window 26 which corresponds in size to the desired cone of rays 25. At each axial end of the cylindrical portion of shield 11 there is an integral bounding portion (such as 15 at the anode end) extending in a generally radial direction.