Patent Grant
8598790
This application claims priority of European Patent Application No. 11161779.1 filed on Apr. 8, 2011.
The invention relates to an electron accelerator of the re-circulating type and sometimes referred to as a Rhodotron® because the trajectory followed by the electrons in the accelerator has the shape of a flower (“Rhodos” means flower in Greek).
The invention more particularly relates to an electron accelerator comprising:
Such accelerators are known from European patent number EP-359774 and from European patent number EP-694247.
The resonant cavity of these known electron accelerators is energized by a high-frequency high-power RF source (hereafter the RF system) operating in the VHF frequency range, generally around 100 MHz or around 200 MHz, and delivering an output RF power which can reach several hundreds of kilowatts.
Such known RF system typically comprises an oscillator for generating an RF signal at the desired frequency, followed by a chain of amplifiers for achieving the desired output RF power at the end of the chain. A final amplification stage in the chain comprises a final power amplifier (often referred to as an FPA) which is coupled to the resonant cavity so that the appropriate transverse electric field is generated inside the cavity.
A central component of such an FPA is typically a high-power high-frequency vacuum tube, such as a tetrode or a Diacrode® for instance. When in operation, this vacuum tube is submitted to very high thermal constraints and must be appropriately cooled down during operation. A failure in the cooling system for instance will quickly lead to a destruction of the tube by overheating, which would for instance lead to ceramics breakage. Furthermore, the high RF currents flowing across the tube electrodes may melt the socket contacts if those contacts are loose or damaged.
It goes without saying that the accelerator will be totally out of order if the vacuum tube of the FPA breaks down. This negatively affects users of the accelerator, all the more since replacing the vacuum tube of the FPA is a delicate and time-consuming task.
Such an accelerator is also known from international patent publication number WO2008/138998 which discloses a cavity equipped with two FPAs, each of which being separately coupled to the cavity through an individual inductive loop. Such a configuration may or may not work well, depending on parameters which are not disclosed in this document.
It is an object of the invention to provide an electron accelerator which is more reliable and/or more robust than the existing accelerators.
To this end, the electron accelerator according to the invention is characterised in that the individual inductive loops are physically spaced apart from each other by an angle alpha, such that alpha is not an integer multiple of 90 degrees.
The inventors have indeed found that, surprisingly, thanks to such a geometrical arrangement of the inductive loops, the cavity will be less prone to be excited according to unwanted resonance modes (i.e. modes which would not provide the electric field which is typically required for accelerating the electrons in the cavity according to the above mentioned flower-shaped trajectory), which would otherwise degrade the performance of the accelerator or even lead to no performance at all.
As an additional advantage of providing a plurality of FPAs (in particular: more than two FPAs), it becomes possible to provide a scalable accelerator. Indeed, an accelerator designed for delivering a maximum beam power can for example initially be equipped with one or two FPA delivering a fraction of the RF power needed for delivering the maximum beam power, and it can later be completed, without too much design change, with (an) additional FPA(s) for delivering increased beam power up to the maximum beam power.
In this context of costs, it is worthwhile to notice that the cost of the FPA represents an important part of the total cost of the accelerator. This is particularly true for very high power accelerators such as those requiring an RF power in the range of 1000 KW for instance. Vacuum tubes which are capable of delivering such high RF powers are very unique and hence very expensive. Now, by dividing this total RF power among a plurality of FPAs, it becomes possible to make use of lower power and more commonly available vacuum tubes, the cost of which, when multiplied by the number of FPAs needed for reaching a nominal power, being lower than that of a single high power tube of that nominal power. Hence a lower cost RF system can be obtained.
Preferably, the number of final power amplifiers is an odd number. The inventors have indeed found that the cavity will in such a case be even less prone to be excited according to unwanted resonance modes.
In a most preferred case, the number of final power amplifiers is equal to three and in their corresponding individual inductive loops are physically spaced apart from each other by an angle of 120 degrees.
These and further aspects of the invention will be explained in greater detail by way of example and with reference to the accompanying drawings in which:
a and 1b schematically show a prior art electron accelerator;
a and 2b schematically show an electron accelerator according to the invention;
The figures are not drawn to scale. Generally, identical components are denoted by the same reference numerals in the figures.
a schematically shows a prior art electron accelerator. It comprises a resonant cavity (10) having an outer cylindrical conductor (11) of axis (A) and an inner cylindrical conductor (12) having the same axis (A), both cylindrical conductors being shorted at their ends with respectively a top conductive closure (13) and a bottom conductive closure (14). It furthermore comprises an electron gun (20) which is adapted to inject a beam of electrons into the resonant cavity (10) following a radial direction in a median transversal plane (MP) of the resonant cavity (10), and an RF system (50) adapted to generate a resonant transverse electric field of the “TE001” type into the resonant cavity (10) for accelerating the electrons of the electron beam (40) a plurality of times into the median transversal plane (MP) and according to successive trajectories following angularly shifted diameters of the outer cylindrical conductor (11). Conventionally, the “TE001” mode means that the electric field is transverse (“TE”), that said field has a symmetry of revolution (first “0”), that said field is not cancelled out along one radius of the cavity (10) (second “0”), and that there is a half-cycle of said field in a direction parallel to the axis A of the cavity (10).
b schematically shows a cross section of the accelerator of
The accelerator also comprises deflecting magnets (30) for bending back the electron beam (40) emerging from the outer cylindrical conductor (11) and for redirecting the beam towards the axis A.
The RF system (50) of such a known accelerator typically comprises an oscillator for generating an RF signal at the desired frequency, followed by a chain of amplifiers for achieving the desired output power at the end of the chain. A final amplification stage in the chain comprises a final power amplifier (FPA) which is coupled to the resonant cavity (10) for energizing the cavity (10) so that the appropriate transverse electric field is generated in the cavity (10) when the RF system (50) is put into operation.
Such an accelerator is well known in the art, for example from European patent number EP-0359774 and from American U.S. Pat. No. 5,107,221, and it will therefore not be described in further detail here.
a schematically shows an electron accelerator (100) according to the invention. Except for the RF system (50), the structure and operation of this accelerator (100) is similar to that of
Of interest here is the RF system (50) of the accelerator. As with the known accelerators, the RF system (50) comprises an oscillator, such as a voltage controlled oscillator (VCO) for example, which generates a low power (a few Watts for instance) RF signal at the desired frequency, which is a resonance frequency of the cavity (10), for example at 107.5 MHz or at 215 MHz. This oscillator feeds a pre-amplifier stage (52) which is designed to amplify the low power RF signal up to a higher intermediate power.
According to the invention, the intermediate power RF signal is then fed to the inputs of a plurality of Final Power Amplifiers (FPA1, . . . , FPAn) for further increasing the power of the RF signal to a desired output RF power. As shown on
b schematically shows a top view of the accelerator (100) of
The following table gives a few examples of accelerator specifications in case the accelerator is equipped with a coaxial cavity (10) of 2 m diameter resonating at 107.5 MHz in the λ/2 mode and with an RF system (50) having various numbers of FPAs, each FPA yielding an output RF power of 280 KW:
The individual inductive loops (55) are physically spaced apart from each other by an angle α (alpha) which is not an integer multiple of 90 degrees. In other words, the inductive loops (55) are neither spaced apart by 90 degrees, nor by 180 degrees, nor by 270 degrees.
Preferably, the number of final power amplifiers (FPA) is an odd number. More preferably, the number of final power amplifiers is equal to three.
Most preferably, the accelerator (100) comprises exactly three FPAs and their corresponding individual inductive loops (55) are physically spaced apart from each other by an angle of 120 degrees.
The RF system (50) is here equipped with a plurality of parallel amplification branches, in this example three branches comprising each a chain of three intermediate amplifiers (5211, 5212, 5123; 5221, 5222, 5223; 5231, 5232, 5233) and ending each with an FPA (FPA1, FPA2, FPA3) inductively coupled to the cavity (10) with their respective individual inductive loops (541, 542, 543) as explained here above. Each branch is fed with substantially the same RF signal originating from the oscillator (51).
Except for one branch (the left branch on the example of
The selection of the appropriate time delays can be performed for example by first switching on the first FPA (the one without delay line and which is supposed to be a reference for the synchronization with the electron gun (20)), by then switching on a second FPA (one with a delay line) and by tuning its delay line (702) until the anode current of the second FPA's vacuum tube becomes minimum, and to repeat the previous step for all FPAs.
Preferably, a variable attenuator (802, 803) is placed upstream of each delay line (702, 703). In this manner, the corresponding FPAs (FPA2, FPA3) can be driven progressively. In the second step of the above synchronization method, the second FPA (FPA2) can then for example be switched on progressively, i.e. by first setting a maximum attenuation and by progressively reducing the attenuation. The same may hold for the third step of the method.
The FPA comprises a high power vacuum tube (60), in this case a tetrode (60) having an anode (An), a cathode (K), a control grid (G1) and a screen grid (G2). The cathode (K) receives the RF signal (VRFin) from the pre-amplification stage (52) (L1 and L2 represent line impedances). The RF signal at the anode (VRFout) is first DC-blocked through capacitor (C2) and then coupled to the resonant cavity (10), here represented by a parallel resonant LC circuit (Lcav, Ccav), through a λ/4 resonant inductive loop (λ being the wavelength of the RF signal) made up of a capacitor (C4), a short transmission line (54) and an inductive loop (55) inside the cavity (10). Such kind of coupling provides for a substantially constant ratio between the transverse electric field in the cavity (10) and the RF voltage on the anode of the tetrode (60) (VRFout). By this method, the load of the FPA shows up as variable resistance for the tetrode (60), so that it can operate at peak efficiency whatever the load.
The anode (An) furthermore receives a high DC voltage (VA) of 16 KV for instance. The control grid (G1) is polarized to a negative DC voltage VG1 of −300 V for instance, for operation of the FPA in the AB class. Capacitor C1 allows to put the control grid (G1) to the mass at the RF frequency. The screen grid (G2) is polarized to a positive DC voltage VG2 of +1000 V for instance. A part of the RF signal is fed back to the screen grid (G2) via capacitor C3. The cathode is directly heated by an additional power source (not shown).
In the figures, the power supplies for powering the various components of the RF system were not shown for clarity reasons. A single power supply with various power converters can be used for powering the various FPAs. Nevertheless, each final power amplifier (FPA1, FPA2, . . . ) of the RF system (50) is preferably provided with its own individual and independent power supply, so that the failure of one such power supply does not negatively affect the operation of the other FPAs.
The present invention has been described in terms of specific embodiments, which are illustrative of the invention and not to be construed as limiting. More generally, it will be appreciated by persons skilled in the art that the present invention is not limited by what has been particularly shown and/or described hereinabove. The invention resides in each and every novel characteristic feature and each and every combination of characteristic features. Reference numerals in the claims do not limit their protective scope. Use of the verbs “to comprise”, “to include”, “to be composed of”, or any other variant, as well as their respective conjugations, does not exclude the presence of elements other than those stated.
Use of the article “a”, “an” or “the” preceding an element does not exclude the presence of a plurality of such elements.
Summarized, the invention may also be described as follows: an electron accelerator (100) of the re-circulating type, sometimes also called a Rhodotron®, comprising a resonant coaxial cavity (10) presenting an outer cylindrical conductor (11) of axis A and a coaxial inner cylindrical conductor (12), an electron gun (20) for injecting electrons (40) into the cavity following a radial direction and into a median transversal plane (MP) of the cavity (10), an RF system (50) for generating a transverse electric field into the cavity which is capable of accelerating the injected electrons (40) following a trajectory into the median plane (MP) which has the shape of a flower centered on the axis A, deflecting magnets (30) disposed into the median plane (MP) externally to—and around the cavity (10) for redirecting electrons (40) emerging from the outer cylindrical conductor (11) back towards the axis A. The RF system comprises a plurality of final power amplifiers (FPA1, FPA2, . . . , FPAn), each said amplifier being directly coupled to the cavity (10) through its own individual inductive loop (55), and each two of these loops being physically spaced apart from each other by an angle alpha, such that alpha is not an integer multiple of 90 degrees so as to reduce the risk of the cavity being excited according to undesired modes.
Such electron accelerators may be used for the irradiation of various substances, such as agro-alimentary products, either directly by the accelerated electrons or indirectly by X-rays produced by said electrons after hitting a metal target for instance.
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