The present invention relates generally to generation of x-rays, and more particularly to a tribocharging x-ray transmitter.
X-rays are used in a variety of ways. X-rays may be used for medical or other imaging applications, crystallography related applications including material analysis, or in other applications.
X-rays are generally generated by electron braking (bremmstrahlung) or inner shell electron emission within a material. Historically, other than through natural phenomena, x-rays generally have been generated by accelerating electrons into a material, such as a metal, with a small proportion of the electrons causing x-rays through bremmstrahlung or knocking electrons present in the material out of inner orbitals, for example K-shell orbitals, with x-rays being generated as electrons in higher energy orbitals transition to the lower energy orbitals. Acceleration of the electrons to generate a useful quantity of x-rays, however, generally requires high powered electrical energy sources, which may include bulky equipment.
X-rays may also be generated by changes in mechanical contact between materials in a controlled environment, for example through the unpeeling of pressure sensitive adhesive tape or mechanical contact of some materials in an evacuated chamber. However, changing mechanical contact between materials generally involves moving parts within the evacuated chamber, and generally also requires that some of the moving parts frictionally contact one another. The moving parts and the frictional contact may result in outgassing and production of free debris in the evacuated chamber, possibly impacting operation of such a device.
Aspects of the invention provide an x-ray emitter which may be of a compact design. In some embodiments a small housing, maintaining a low fluid pressure environment therein, has a first wall with a substantially x-ray transparent window with an interior coated with a metal and a second wall with at least a portion of an exterior surface formed of an electrical insulator, preferably a dielectric material. The metal on the window provides an electron target, and alternatively the electron target may instead be positioned within the housing. The portion of the wall may be the dielectric material itself, or the portion of the wall may be a metal, otherwise electrically insulated from the rest of the housing, with a dielectric exterior covering. A contacting material, preferably higher in a triboelectric series, is in changing contact with the exterior covering, with the changing contact preferably being intermittent contact as well. A filament, preferably heatable and preferably metallic, is within the housing, for example proximate the second wall. In operation contact, removal of contact between the contacting material and the dielectric generates a negative electrical charge on the portion of the second wall, particularly an interior surface of the portion of the second wall. Electrons associated with the negative charge, and/or electrons provided by the filament may travel to and impact the metal on the interior of the substantially x-ray transparent window, generating x-rays which are emitted or transmitted through the window.
Some aspects of the invention provide an x-ray emission device, comprising: a housing configured to maintain a low fluid pressure environment, the housing having a first wall with a window substantially transparent to x-rays and a second wall having a portion comprising an exterior surface comprising an electrically insulating material; an electron target comprised of a metal within the housing; an electrically chargeable material within the housing; and a contact material for frictionally contacting the electrically insulating material, the contact material being lower in a triboelectric series than the electrically insulating material.
Some aspects of the invention provide a method of emitting x-rays from a housing, the housing being substantially opaque to x-rays and having a chamber at a low fluid pressure, comprising: frictionally contacting an exterior surface of the housing with a contacting surface, the exterior surface and the contacting surface being of different materials, whereby a charge imbalance is generated through the frictional contact, with accumulation of negative charge by the exterior surface; allowing for a flow of electrons, from about an interior surface of the housing proximate the exterior surface contacted by the contacting surface, and towards a window of the housing; generating x-rays proximate the window of the housing, the window of the housing being substantially transparent to x-rays.
Some aspects of the invention provide a device for emission of x-rays, comprising: a housing configured to maintain a low fluid pressure in a chamber within the housing, the housing including a window substantially transparent to x-rays but otherwise substantially opaque to x-rays; means for generating a charge imbalance on a portion of the housing through changing contact of material external to the housing with a surface of the housing; an electron target within the housing; and a filament within the housing substantially between the portion of the housing and the electron target.
These and other aspects of the invention are more fully comprehended upon review of this disclosure.
The housing has a first wall 113 with at least a portion having an electrically insulating exterior surface, a polyimide film, for example Kapton, in some embodiments, and preferably a dielectric material. In some embodiments the portion of the wall having the electrically insulating exterior is a membrane formed of the electrically insulating exterior. In some embodiments the portion of the wall comprises a metal, electrically insulated from other portions of the housing, towards an interior of the housing, with the electrically insulating material covering the metal on the exterior of the housing. In some embodiments the portion of the housing comprises a grid of metals, which may in some embodiments be within, upon or floated on other material. In some embodiments the portion of the wall comprises a non-metal, for example a glass or a ceramic material.
A contacting surface 115 is in changing contact with the electrically insulating exterior of the housing. The contacting surface is preferably of a material such that changing contact between the contacting surface and the electrically insulating material generates a charge imbalance. Preferably, the material is such that the electrically insulating material becomes more negatively charged. In some embodiment the material is higher in a triboelectric series than the electrically insulating material. The contacting surface may be in changing contact with the electrically insulating material by way of frictional contact of the contacting surface over varying surface areas of the electrically insulating material. This may be accomplished, for example, by having different portions of the contacting surface in contact with different portions of the electrically insulating material over time, by way of repetitive contact and separation of the surfaces, or by way of some or all of the foregoing.
The contacting surface may be moved, or driven, in a variety of manners. In some embodiments, and as representatively illustrated in
In operation, the changing contact between the contacting surface and the electrically insulating material results in electron accumulation, or negative charging, of the electrically insulating material. In embodiments in which the electrically insulating material is a membrane forming a portion of the wall of the housing, the membrane becomes negatively charged. In embodiments in which the electrically insulating material is an exterior cover for a section of the housing, for example a metal section, electrically insulated from other portions of the housing, forming the second wall, the metal becomes negatively charged. The electrons providing the negative charge may travel to and strike an electron target within the housing.
In the embodiment of
Interior to the membrane, and interior to the metal underlying the membrane, if present, are field emitting tips 323. The field emitting tips may be, for example, sharp metal tips or carbon nanotubes. In some embodiments the field emitting tips extend from etal pieces interior to the membrane. In some embodiments there are a plurality of such metal pieces, which in some embodiments are electrically insulated from each other. In some embodiments one field emitting tip extends from each metal piece, in some embodiments one or more field emitting tips extend from each metal piece, and in some embodiments a plurality of field emitting tips extend from each metal piece. Further, in some embodiments a conductive mesh may be placed over the field emitting tips, with a relatively low voltage, less than 1000 V in some embodiments, applied to the conductive mesh to assist in preventing electrical discharge from the field emitting tips; with control of the applied voltage serving to control the electron emission from the tips. A heatable filament 325, for example of tungsten or Lanthanum Hexoboride, or alternatively a cathode such as a Barium Oxide cathode, is also interior of the housing, preferably proximate the field emitting tips. The heatable filament may be coupled to an energy source, for example a battery, through ports (not shown) in the housing. The heatable filament provides an electron source, for example that can be under controlled power from an external power supply.
Another wall of the housing, shown opposite the wall with the dielectric in
Operation of the device of
In the device of
A solid electron target 521, for example of a metal, is in the interior of the housing. The electron target includes a surface 523 having a line of sight with both the filament/field emitting tips/membrane and the window. As the device is operated, electrons from the filament strike the electron target, generating x-rays, some of which exit through the window. Advantageously, in some embodiments the electron target may be rotated such that the surface 523 may receive fewer electrons, or rotated so as to emit fewer x-rays towards the window, allowing for increased control of x-ray flux through the window. Similarly, or additionally, in some embodiments the electron target may be moved closer to or farther from the window, also allowing for increased control of x-ray flux through the window. The distance from the membrane to the target can also be varied, in some embodiments, to change the maximum energy of the striking electrons as a means to control the output x-ray energy. The material of the target can be chosen to provide a particular x-ray spectrum, with for example the characteristic x-ray lines of a material such as Molybdenum. Further, in some embodiments the portion of the housing and the contacting surface, and the field emitting tips, may be instead or in addition be placed in reverse, with these items instead or in addition placed on an opposing side of the housing and the materials of the exterior of the portion of the housing and the contacting surface reversed. With the materials reversed, in operation a positive charge is generated, and with the positive charge attracting electrons from the filament to that opposing side of the housing, with in some embodiments the electron target in the path of such electrons. In some embodiments, however, the electron target may be elsewhere, for example on an interior surface of the window, with what may be considered back scattered electrons generating x-rays in the electron target, with x-rays emitted through the window.
The membrane is negatively tribocharged through rolling contact with a contacting material 615. Material of the membrane and the contacting material are selected such that tribocharging occurs through changing contact of surfaces of the two materials, with the membrane being negatively charged compared to the contacting material.
In the embodiment of
The contacting material is mounted to a base 817 on a drive system. As shown in the embodiment of
As illustrated in
Although the invention has been discussed with respect to various embodiments, it should be recognized that the invention comprises the novel and non-obvious claims supported by this disclosure.
Number | Name | Date | Kind |
---|---|---|---|
2810077 | Gale | Oct 1957 | A |
3612918 | Willutzki | Oct 1971 | A |
3934164 | Braun et al. | Jan 1976 | A |
4789802 | Miyake | Dec 1988 | A |
4990813 | Paramo | Feb 1991 | A |
5665969 | Beusch | Sep 1997 | A |
6353658 | Trebes et al. | Mar 2002 | B1 |
6476406 | Struye et al. | Nov 2002 | B1 |
6493423 | Bisschops | Dec 2002 | B1 |
6668039 | Shepard et al. | Dec 2003 | B2 |
6925151 | Harding et al. | Aug 2005 | B2 |
7060371 | Akiyama et al. | Jun 2006 | B2 |
7596242 | Breed et al. | Sep 2009 | B2 |
20030021377 | Turner et al. | Jan 2003 | A1 |
20060056595 | Sampayon | Mar 2006 | A1 |
20070110217 | Ukita | May 2007 | A1 |
20090050847 | Xu et al. | Feb 2009 | A1 |
20090090875 | Gelbart et al. | Apr 2009 | A1 |
20090238340 | Okada et al. | Sep 2009 | A1 |
20110130613 | Putterman et al. | Jun 2011 | A1 |
Number | Date | Country |
---|---|---|
0833365 | Dec 2003 | EP |
WO 2013-032020 | Mar 2013 | WO |
Entry |
---|
Stefan Kneip, A stroke of X-ray, May 26, 2011, Nature, vol. 473, 455-456. |
Hird et al., A triboelectric x-ray source, Mar. 28, 2011, Applied Physics Letters 98, 133501-1-3. |
Klyuev et al., “The effect of air pressure on the parameters of x-ray emission accompanying adhesive and cohesive breaking solids”, Sov. Phys. Tech. Phys., vol. 34, Mar. 1989, pp. 361-364. |
Nakayama et al., “Triboemission of charged particles and photons from solid surfaces during frictional damage”, Journal of Physics D. Applied Physics, vol. 25, No. 2, Feb. 14, 1992, pp. 303-308. |
Nishitani et al., “STM tip-enhanced photoluminescence from porphyrin film”, Surface Science, North-Holland Publishing Co., vol. 601, No. 17, Aug. 23, 2007, pp. 3601-3604. |
Ohara et al., “Light emission due to peeling of polymer films from various substrates”, Journal of Applied Polymer Science, vol. 14, No. 8, Aug. 1, 1970, pp. 2079-2095. |
International Search Report on related PCT Application No. PCT/US2014/027795 from International Searching Authority (KIPO) dated Jul. 11, 2014. |
Written Opinion on related PCT Application No. PCT/US2014/027795 from International Searching Authority (KIPO) dated Jul. 11, 2014. |
Number | Date | Country | |
---|---|---|---|
20140270088 A1 | Sep 2014 | US |