The present application is related generally to high voltage power supplies for x-ray sources.
A power supply can provide electric power to operate an electron-emitter in an x-ray tube. Feedback from the electric circuit to the power supply can adversely affect power supply operation. It would be beneficial to avoid this undesirable noise in the power supply. Electric power can be lost (I2*R) due to resistance of wires between the power supply and the x-ray tube. It would be beneficial to minimize this power loss. It can be important to reduce x-ray source size and cost, especially for portable x-ray sources.
It has been recognized that it would be advantageous to provide more efficient power transfer to the electron-emitter and avoid undesirable noise in the power supply. It has been recognized that it would be advantageous to reduce the size and cost of cables between the power supply and the x-ray tube.
The present invention is directed to various embodiments of an x-ray source and a power supply for an x-ray tube, which satisfy these needs. Each embodiment may satisfy one, some, or all of these needs.
The power supply for the x-ray tube can comprise a control box and a remote box. The control box can be electrically coupled to the remote box by a relatively long box-connector cable. A high voltage source can be configured to provide a bias voltage to an electron-emitter, an anode, or both, in the x-ray tube. The high voltage source can be located in the control box or in the remote box. The control box can include an alternating current (AC) source configured to provide AC for the electron-emitter; an electron-emitter controller configured to control the AC source; and a high voltage controller configured to provide electrical power to operate the high voltage source. The remote box can include an electron-emitter transformer. The electron-emitter transformer can include primary windings and secondary windings. The primary windings can be electrically coupled to the AC source and can be configured to transfer an AC signal from the AC source to the secondary windings. The secondary windings can be configured to be electrically coupled across the electron-emitter.
The x-ray source can include a power supply, similar to that just described, plus an x-ray tube including (1) a cathode and an anode, electrically insulated from each other; (2) the cathode including an electron-emitter capable of emitting electrons towards the anode; and (3) the anode capable of emitting x-rays in response to impinging electrons from the electron-emitter.
Wires or cables can be used to transfer alternating current (AC). If short cables transfer AC, then the cables are regarded merely as conductors, and the cables have minimal effect on the circuit except for transfer of electrical current. If long cables transfer AC, then the cables are regarded as a transmission line and distributed inductance and distributed capacitance of the cables can affect the electrical circuit. Generally, cables are considered to be long if the cable is longer than one fourth of a wavelength of the AC signal.
If a transmission line is terminated by a load with impedance equal to the characteristic impedance of the transmission line, then no power is reflected back to the electrical power source and there can be maximum transfer of power to the load. If, however, the load impedance does not equal the characteristic impedance, then electrical power will be at least partially reflected back to the electrical power source, resulting in inefficient transfer of power and possibly undesirable noise in the power supply.
Shown in
A high voltage controller 16 can provide electrical power (e.g. AC) to a high voltage source 15. The high voltage source 15 can then provide a large negative bias voltage (e.g. ≦−4 kV) to the electron-emitter 19. The high voltage source 15 can be a high voltage multiplier, such as for example, a Cockcroft-Walton multiplier.
In one application using x-ray source 10, the AC signal wavelength is 4000 meters. X-ray source 10 users desire a distance between the power supply 17 and the electron-emitter 19 of about 2-5 meters to position the x-ray tube in a very small space where the power supply 17 cannot fit. Thus, these users desire an x-ray tube cable 21 (cable between the electron-emitter transformer 14 and the electron emitter 19) with a length L1 of about 2-5 meters. The longest desired x-ray tube cable 21 is less than ¼ of the AC signal wavelength (1/4*4000 m=1000 m), so it appears that the x-ray tube cable 21 can be treated as a short cable, i.e. merely as a conductor and not as a transmission line.
The desired waveform of the voltage through electron-emitter transformer 14 is the square waveform shown in
A cause of the relatively short x-ray tube cable 21 acting as a transmission line is believed to be the AC source design. The AC source 22 design, which is useful for portable x-ray sources, causes a change of the transition point from cable to transmission line. Lowering the frequency of the AC signal can extend this transition point further out, and possibly allow the use of cables with a length up to or greater than the desired 5 meters, but lowering the frequency can cause inefficient operation of the electron-emitter transformer 14. Matching the electron-emitter 19 impedance with the characteristic impedance of the x-ray tube cable 21 can allow efficient transfer of AC, but such matching is not practical in this circuit (electron-emitter 19 design is set based on desired x-ray emission). Thus, another solution is desired for efficient power transfer to the electron-emitter 19 without undesirable noise in the power supply 17.
Another problem of x-ray source 10 is electrical power loss in the x-ray tube cable 21. A high electrical current may be needed for the electron-emitter 19 (e.g. to heat filaments). Electrical power loss due to this high electrical current can result in high power losses (P=I2*R).
An additional problem of x-ray source 10 is size and cost of the x-ray tube cable 21. This problem is more troublesome if the x-ray source 10 has a relatively high bias voltage and/or a relatively long x-ray tube cable 21.
Illustrated in
The x-ray sources 40, 50, 60, 70, 80, and 90 can include a power supply 17 and an x-ray tube 49. The x-ray sources 40, 50, 60, 70, 80, and 90 can be battery-operated (i.e. a battery supplies electric power to the power supply) and can be portable. The x-ray tubes 49 shown in the figures are transmission-target type, but the invention herein is applicable also to side-window x-ray tubes.
The power supply 17 can include a control box 48 and a remote box 47. The control box 48 can be electrically coupled to the remote box 47 by a box-connector cable 41. The box-connector cable 41 can include a connector 46 to allow connection and disconnection of the remote box 47 to the control box 48. The box-connector cable 41 can provide electrical power for an electron-emitter 19 and also can include a ground cable (not shown).
The remote box 47 can be electrically coupled to the x-ray tube 49 by an x-ray tube cable 21. The x-ray tube cable 21 can include a connector 38 to allow connection and disconnection of the remote box 47 to the x-ray tube 49. The x-ray tube cable 21 can also include a ground cable (not shown).
The x-ray tube 49 can include a cathode 42 and an anode 43 which can be electrically insulated from each other (e.g. by an electrically insulative enclosure 39). The cathode 42 can include an electron-emitter 19 which can emit electrons 45 towards the anode 43. The anode 43 can emit x-rays 44 in response to impinging electrons 45 from the electron-emitter 19.
A high voltage source 15 can be located in the control box 48 (see
The high voltage source 15 can provide a large negative bias voltage to the electron-emitter 19 (see
The high voltage source 15 can provide a large positive bias voltage to the anode 43 (see
The high voltage source 15 can provide a large negative bias voltage to the electron-emitter 19 and a large positive bias voltage to the anode 43 (see
The control box 48 can include an AC source 22 for the electron-emitter 19, an electron-emitter controller 11, and a high voltage controller 16. In some designs, the control box 48 can also include the high voltage source 15 (see
The high voltage controller 16 can provide electrical power to operate the high voltage source 15. For example, if the high voltage source 15 is a Cockcroft-Walton multiplier, then the high voltage controller 16 can provide AC, at a desired amplitude and frequency, to the high voltage source 15, to obtain the desired output DC bias voltage.
The remote box 47 can include an electron-emitter transformer 14. In some designs, the remote box 47 can also include the high voltage source 15, as shown in
In the design shown in
The relatively long box-connector cable 41 can allow the x-ray source user to locate the x-ray tube 49 in remote locations. The remote box 47 can be small enough to fit into small locations with the x-ray tube 49 because the remote box 47 might only contain the electron-emitter transformer 14 and possibly also the high voltage source 15. A size of the remote box 47 can be less than 50 cm3 in one aspect, less than 20 cm3 in another aspect, less than 10 cm3 in another aspect, or less than 5 cm3 in another aspect.
The x-ray tube cable 21 can be relatively short. For example, the x-ray tube cable 21 can have a length of less than 0.75 meters in one aspect, less than 0.5 meters in another aspect, or less than 0.25 meters in another aspect.
It can be relatively easy to substantially match a characteristic impedance of the box-connector cable 41 to the load seen at the electron-emitter transformer 14 by adjusting the turns of the primary windings 14p, but it can be more difficult or impractical to match characteristic impedance of the x-ray tube cable 21 to the electron emitter 19. Thus, there can be efficient electrical power transfer from the control box 48 to the remote box 47 without undesirable noise by matching or approximately matching the characteristic impedance of the box-connector cable 41 to the load seen at the electron-emitter transformer 14. There can be efficient electrical power transfer from the remote box 47 to the x-ray tube 49, even if characteristic impedance of the x-ray tube cable 21 does not match impedance of the electron-emitter 19, because the x-ray tube cable 21 can be relatively short.
A high turn ratio of primary windings 14p to secondary windings 14s on the electron-emitter transformer 14 can also improve electrical power transfer. AC can be transferred on the relatively long box-connector cable 41 at a higher voltage in order to reduce power loss, then stepped down at the electron-emitter transformer 14 for transfer of electrical power through the possibly short x-ray tube cable 21 to the electron-emitter 19. For example, a turn ratio of primary windings 14p to secondary windings 14s on the electron-emitter transformer 14 can be: ≧2:1 in one aspect or ≧4:1 in another aspect and can be ≦10:1 in one aspect or ≦20:1 in another aspect.
As shown in
As shown in
A first bias wire 68 can electrically couple the high voltage source 15 and the output windings 64o to provide the negative bias voltage to the output windings 64o. The first bias wire 68 can be short (e.g. less than 5 centimeters) and can be located entirely within the control box 48. A second bias wire 69 can electrically couple the primary windings 14p and the secondary windings 14s to transfer the negative bias voltage from the primary windings 14p to the secondary windings 14s. The second bias wire 69 can be short (e.g. less than 5 centimeters) and can be located entirely within the remote box 47.
An advantage of x-ray sources 50, 60, and 70 over x-ray source 80 is only one transformer between the electron-emitter 19 and the AC source 22. A disadvantage of x-ray sources 50, 60, and 70 in comparison to x-ray source 80 is that the DC bias cable 18 in x-ray sources 50, 60, and 70 can be larger and more expensive. The advantages of each design can be compared for each use.
As shown on x-ray source 90 in
This application claims priority to U.S. Provisional Patent Application No. 62/191,242, filed on Jul. 10, 2015, which is hereby incorporated herein by reference in its entirety.
Number | Date | Country | |
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62191242 | Jul 2015 | US |