This disclosure relates to an X-ray tube anode target assembly and, more particularly, to configuration and structures for controlling heat dissipation and structural loads for an X-ray tube anode target assembly.
Ordinarily an X-ray beam-generating device referred to as an X-ray tube comprises dual electrodes of an electrical circuit in an evacuated chamber or tube. One of the electrodes is electron emitter cathode which is positioned in the tube in spaced relationship to a target anode. Upon energization of the electrical circuit generates a stream or beam of electrons directed towards the target anode. This acceleration is generated from a high voltage differential between the anode and cathode that may range from 60-450 kV, which is a function of the imaging application. The electron stream is appropriately focused as a thin beam of very high velocity electrons striking the target anode surface. The anode surface ordinarily comprises a predetermined material, for example, a refractory metal so that the kinetic energy of the striking electrons against the target material is converted to electromagnetic waves of very high frequency, i.e. X-rays, which proceed from the target to be collimated and focused for penetration into an object usually for internal examination purposes, for example, industrial inspection procedures, healthcare imaging and treatment, or security imaging applications, food processing industries. Imaging applications include, but are not limited to, Radiography, CT, X-ray Diffraction with Cone and Fan beam x-ray fields.
Well-known primary refractory and non-refractory metals for the anode target surface area exposed to the impinging electron beam include copper (Cu), Fe, Ag, Cr, Co, tungsten (W), molybdenum (Mo), and their alloys for X-ray generation. In addition, the high velocity beam of electrons impinging the target surface generates extremely high and localized temperatures in the target structure accompanied by high internal stresses leading to deterioration and breakdown of the target structure. As a consequence, it has become a practice to utilize a rotating anode target generally comprising a shaft supported disk-like structure, one side or face of which is exposed to the electron beam from the thermionic emitter cathode. By means of target rotation, the impinged region of the target is continuously changing to avoid localized heat concentration and stresses and to better distribute the heating effects throughout the structure. Heating remains a major problem in X-ray anode target structures. In a high speed rotating target, heating must be kept within certain proscribed limits to control potentially destructive thermal stresses particularly in composite target structures, as well as to protect low friction, solid lubricated, high precision bearings that support the target.
Only about 1.0% of the energy of the impinging electron beam is converted to X-rays with the remainder appearing as heat, which must be rapidly dissipated from the target essentially by means of heat radiation. Accordingly, significant technological efforts are expended towards improving heat dissipation from X-ray anode target surfaces. For most rotating anode targets heat management must take place principally through radiation and a material with a high heat storage capacity. Stationary anode target body configurations or some complex rotating anode target configurations may be designed to have heat transfer primarily take place using conduction or convection from the target to the x-ray tube. Life of rotating x-ray targets are often gated by the complexities of rotation in a vacuum. Traditional x-ray target bearings are solid lubricated, which have relatively low life. Stationary targets do not have this life-limiting component, at the cost of lower performance.
Other rotation components, solid lubricated bearings, ferro-fluid seals, spiral-grooved liquid metal bearings, etc, all introduce manufacturing complexity and system cost.
What is needed is a high flux X-ray tube configuration that provides improved heat dissipation and includes components capable of maintaining an extended life, with a limited introduction of cost and manufacturing complexity.
One aspect of the present disclosure includes an X-ray tube anode assembly having a movable X-ray target having a target surface. The anode assembly includes a drive member arranged and disposed to provide oscillatory motion to the target assembly and a target surface that is configured to remain at a substantially fixed distance from a cathode assembly during oscillatory motion.
Another aspect of the present disclosure includes an X-ray tube assembly including an envelope having at least a portion thereof substantially transparent to X-ray. The assembly also includes a cathode assembly, operatively positioned in the envelope with an anode assembly having a movable X-ray target having a target surface. The anode assembly includes a drive member arranged and disposed to provide oscillatory motion to the target assembly and a target surface that is configured to remain at a substantially fixed distance from a cathode assembly during oscillatory motion. This anode system may be tuned to allow the pivot to be driven at natural frequency, lowering the required drive power to obtain the desired oscillatory frequency.
Still another aspect of the present disclosure includes a method for providing heat management to an X-ray assembly. The method includes providing an X-ray tube having including an envelope having at least a portion thereof substantially transparent to X-ray. The assembly also includes a cathode assembly, operatively positioned in the envelope with an anode assembly having a movable X-ray target having a target surface. The anode assembly includes a drive member arranged and disposed to provide oscillatory motion to the target assembly and a target surface that is configured to remain at a substantially fixed distance from a cathode assembly during oscillation. The method further includes oscillating the anode assembly, wherein the target surface is configured to remain at a substantially fixed distance from the cathode assembly during the oscillating.
The position of the focal point along the surface of the target is varied, providing improved heat management, wherein the heat may be dissipated more easily. In addition, the increased dissipation permits the use of higher power and longer durations than are available with the use of a stationary anode arrangement. In addition, the anode has increased life over anodes that have a fixed focal point on the anode. The oscillatory motion provides longer life than solid lubricated bearings used in known rotating anode sources.
Additionally, the assembly will have reduced manufacturing complexity, and cost, in comparison to conventional rotational bearing arrangements.
The assembly of the present disclosure may allow multiple spots to be placed on a single target, in that each region will be thermally isolated from the neighboring spot, while maintaining the benefit of higher power through oscillatory motion from a single drive mechanism.
The assembly of the present disclosure may also allow for the introduction of oscillatory motion into an array of focal spots on a multi-spot anode source.
Embodiments of the present disclosure also allow the distribution of heat over a larger area of the anode target, through the oscillating motion, which reduces the peak temperature and maintains the temperature below the evaporation limit for the metal in the envelope, and reduces the temperature gradient between surface and substrate
Other features and advantages of the present disclosure will be apparent from the following more detailed description of the preferred embodiment, taken in conjunction with the accompanying drawings which illustrate, by way of example, the principles of the disclosure.
Wherever possible, the same reference numbers will be used throughout the drawings to refer to the same or like parts.
The cathode assembly 109 comprises an electron emissive portion 111 mounted to a support 113. The disclosure is not limited to the arrangement shown, but may be any arrangement and/or geometry that permits the formation of an electron beam at the electron emissive portion 111. Conductors or other current supplying mechanism may be included in the cathode assembly 109 to supply heating current to a filament and/or conductor present in the cathode assembly for maintaining the cathode at ground or negative potential relative to the target 105 of the tube 100. An electron beam from the electron emissive portion 111 impinges upon target 105 at a focal point on the target focal surface 107 to produce X-radiation (see e.g.,
The oscillation provides movement of the target 105, such that the focal point within the target focal surface 107 provides a substantially constant X-ray emission, wherein the target 105 moves relative to the focal point. Specifically, the drive assembly 101 provides oscillatory motion to target 105 such that the focal point remains at a substantially fixed distance from the electron emissive portion 111 and/or the angle at which the electron beam impinges the target 105 remains substantially constant. The present disclosure is not limited to reflection based geometry for X-ray generation, but may include alternate configurations, such as targets 105 configured for transmission generated X-rays. The anode assembly and the cathode assembly 109 are housed in an envelope 115, which is under vacuum or other suitable atmosphere. One embodiment includes a portion of the drive assembly 101 (e.g. the stator portion) exterior to the envelope. At least a portion of the envelope 115, which acts as a window for the X-rays, is glass or other material substantially transparent to X-rays. The configuration of the envelope 115 may be any configuration suitable for providing the X-radiation to the desired locations and may be fabricated from conventionally utilized materials.
Coupling mechanisms 501, for example, utilizing linear springs to provide oscillation, may have up to infinite life spans for a prescribed radial load and oscillating angle, which life spans are difficult or impossible in known rotary motion assemblies. During operation of X-ray tube 100, the drive assembly 101, which is configured to oscillate the target 105 in a manner that results in flexing of the coupling mechanism 501, which, permits motion of the first segment 401 (i.e. oscillation 402) with respect to the second segment 403. The oscillation of the first segment 401 provides target 105 with oscillatory motion 201 desirable for heat management.
The resultant oscillatory motion 201 provides a path along which the focal point travels. Since the position along the target 105 is varied, the heat generated by the impingement of the electrons on the target 105 is permitted to dissipate over a larger area. This dissipation of heat permits the use of higher power and longer durations than are available with the use of a stationary anode arrangement.
The present disclosure is not limited to oscillation provided through the use of a oscillatory coupling 103, but also includes direct actuation of the target 105 in a oscillatory motion 201. For example, the target 105 may be affixed to a drive assembly 101, wherein the drive assembly 101 provides reciprocating rotation or oscillation of the target 105, such that the target focal surface 107 provides substantially constant production of X-rays from the electron beam 601. Other configurations, such as a linear or elongated target 105 having an oscillated target focal surface 107 actuated by a linear actuator or other linear motion device. Further a cam or similar device may be utilized to translate rotational or other motion to oscillatory motion. In addition, the present disclosure is not limited to the geometry of the targets shown and may include target geometries that are asymmetrical or other non-circular arrangements. Further still, the present disclosure is not limited to a single focal point and may include multiple focal points.
As shown in
An example finite element analysis comparing a stationary target to a oscillating target with +/−9.5° degree oscillation at 10 Hz on a 78 mm radius arc shows an entitlement of 2.3× power increase while maintaining thermal limits of track surface temperature <2400° C. and copper temperatures of <300° C. One skilled in the art would note that the power increase is gated by the optimization of the track oscillation angle, oscillation frequency and focal spot path radii. In addition, the power increase includes varied system size, cost and expected life span. The oscillatory motion introduces transient temperature fields on the surface of the anode target that will have a peak dwell time of the focal beam at the end of the oscillation path. The ends of the oscillation path determine the thermal limit of the track surface.
While the disclosure has been described with reference to a preferred embodiment, it will be understood by those skilled in the art that various changes may be made and equivalents may be substituted for elements thereof without departing from the scope of the disclosure. In addition, many modifications may be made to adapt a particular situation or material to the teachings of the disclosure without departing from the essential scope thereof. Therefore, it is intended that the disclosure not be limited to the particular embodiment disclosed as the best mode contemplated for carrying out this disclosure, but that the disclosure will include all embodiments falling within the scope of the appended claims.
Number | Name | Date | Kind |
---|---|---|---|
1997676 | Catlin | Apr 1935 | A |
2926270 | Zunick | Feb 1960 | A |
3398307 | Brown et al. | Aug 1968 | A |
3836805 | Kok | Sep 1974 | A |
4107563 | Oddell | Aug 1978 | A |
4162420 | Grady | Jul 1979 | A |
4399551 | Grady | Aug 1983 | A |
7042975 | Heuscher | May 2006 | B2 |
7305063 | Heuscher | Dec 2007 | B2 |
7305066 | Ukita | Dec 2007 | B2 |
7394891 | Sakabe | Jul 2008 | B2 |
20050207537 | Ukita | Sep 2005 | A1 |
20090238328 | Forthmann et al. | Sep 2009 | A1 |
20100027753 | Venugpal et al. | Feb 2010 | A1 |
Number | Date | Country |
---|---|---|
29622655 | Jan 1996 | DE |
2001351551 | Dec 2001 | JP |
Number | Date | Country | |
---|---|---|---|
20090074145 A1 | Mar 2009 | US |