Patent Description:
Nuclear fission reactors generate a constant stream of radioactive nuclides of the spent fuel: in United States alone <NUM>,<NUM> metric tons requires disposal [Ref. <NUM>], and by <NUM> the worldwide spent nuclear waste inventory will reach <NUM>,<NUM> metric tons with <NUM> tons added each year. Nuclear power accounts for <NUM>% of electricity in France, making the need for transmutation particularly acute. Currently, there are no proper and adequate means available to treat these isotopic radioactive materials other than deep earth burial. The development of such means to treat isotopic radioactive materials requires the completion of two tasks: First, developing easy, robust, safe, and inexpensive methods to separate highly radioactive isotopes from the rest of the materials in order to avoid activating the non-radioactive material through transmutation; and, second, developing a safe, inexpensive, energy non-exhaustive, versatile transmutation method.

Current approaches to transmutation of radioactive nuclei include drivers that maintain the subcritical fission reactor by an external means: one is based on an accelerator driven system (ADS) [Ref. <NUM>], and the other is based on tokamak driven systems [Ref. <NUM>]. The ADS system relies on a highly energetic (~<NUM> GeV) proton beam impinging on a substrate (e.g. Pb, W) and ejecting neutrons (<NUM>+ neutrons per proton). These neutrons then maintain fission in a subcritical reactor. The tokamak-based system generates neutron from the deuterium-tritium reactions and uses these neutrons to drive the subcritical reactor, also called the fission-fusion hybrid.

Other approaches to transmuting nuclear waste based on a supercritical operation also exist - MOSART [Ref. <NUM>], as well as various approaches using the Gen-IV reactors.

For these and other reasons, needs exist for improved systems, devices, and methods that facilitates generation of a large rate of energetic neutrons by electrostatic accelerator-driven beam for purposes of subcritical liquid phase-based transmutation of radioactive waste. <CIT> discloses a radiocactive waste containing medium is circulated within two or more systems separated from each other flow technically; and the circulated radioactive waste is exposed to neutron radiations of different energy spectrum in each system by operating a reactor physically united entirety of irradiated sections of the said systems as a nuclear reactor or an accelerator driven subcritical system. Each system has a heat exchanger and, in given cases, a circulating pump and an expansion tank. The disclosed apparatus has two or more reactor regions separated from each other by partitions and, preferably, arranged coaxially within a reactor space encircled by a common shell structure. A particle beam produced by a particle accelerator is preferably directed into the innermost reactor region. <CIT> discloses n apparatus for generating medical isotopes provides an annular fissile solution vessel surrounding a neutron generator. The annular fissile solution vessel provides for good capture of the emitted neutrons and a geometry that provides enhanced stability in an aqueous reactor. A neutron multiplier and/or a neutron moderator may be used to improve the efficiency and control the criticality of the reaction in the annular fissile solution vessel.

The present application provides a transmutator system for transmutation of long-lived radioactive transuranic waste in accordance with the claims which follow.

Other systems, devices, methods, features and advantages of the subject matter described herein will be or will become apparent to one with skill in the art upon examination of the following figures and detailed description. It is intended that all such additional systems, methods, features and advantages be included within this description, be within the scope of the subject matter described herein, and be protected by the accompanying claims. In no way should the features of the example embodiments be construed as limiting the appended claims, absent express recitation of those features in the claims.

The details of the example embodiments, including structure and operation, may be gleaned in part by study of the accompanying figures, in which like reference numerals refer to like parts. The components in the figures are not necessarily to scale, emphasis instead being placed upon illustrating the principles of the disclosure. Moreover, all illustrations are intended to convey concepts, where relative sizes, shapes and other detailed attributes may be illustrated schematically rather than literally or precisely.

It should be noted that elements of similar structures or functions are generally represented by like reference numerals for illustrative purpose throughout the figures. It should also be noted that the figures are only intended to facilitate the description of the preferred embodiments.

Each of the additional features and teachings disclosed below can be utilized separately or in conjunction with other features and teachings to provide systems and methods that facilitate the transmutation of long-lived radioactive waste into short-live radioactive nuclides or stable nuclides utilizing an electrostatic accelerator particle beam approach to the generation of neutrons.

Moreover, the various features of the representative examples and the dependent claims may be combined in ways that are not specifically and explicitly enumerated in order to provide additional useful embodiments of the present teachings. In addition, it is expressly noted that all features disclosed in the description and/or the claims are intended to be disclosed separately and independently from each other for the purpose of original disclosure, as well as for the purpose of restricting the claimed subject matter independent of the compositions of the features in the embodiments and/or the claims. It is also expressly noted that all value ranges or indications of groups of entities disclose every possible intermediate value or intermediate entity for the purpose of original disclosure, as well as for the purpose of restricting the claimed subject matter.

In exemplary embodiments provided herein, the neutrons are generated by electrostatic accelerator driven fusion to transmute long lived radioactive nuclei into short-lived or non-radioactive nuclides.

In exemplary embodiments, a transmutation process employees a subcritical method of operation utilizing a compact device to transmute radioactive isotopes (mainly those of minor actinides (MA)) carried out in a tank containing a liquefied solution of a mix of the spent fuel waste components (such as the fission products (FP) and MA) dissolved within molten salt solution of LiF-BeF2 (FLiBe). Such process is described in <CIT> [Ref. <NUM>]. Transmutation of the MA is performed with energetic neutrons originating from a fusion reaction driven by an electrostatic accelerator. Monitoring and control in real-time of the FLiBe, MA and FP content within the transmutator is performed with active laser spectroscopy or a laser driven gamma source.

Turning to the figures, <FIG> show a segmented transmutator vessel <NUM>. <FIG> shows a representative case of axial radial segmentation of the vessel <NUM> into three (<NUM>) vessel sections 100A, 100B and 100C. <FIG> shows a representative cross-section of the radial and azimuthal segmentation of the vessel <NUM>. The transmutator vessel <NUM> in the present embodiment is radially segmented into concentric cylindrical chambers or tanks <NUM>, <NUM>, <NUM>, <NUM> and <NUM>. An azimuthally segmented chamber <NUM> shows a representative chamber used for either diagnostics or for additional source of neutrons. By segmenting the vessel <NUM>, control and localization of various parameters can be increased more easily and/or more precisely, as well as increase the overall transmutator safety by data feedback from various segments via an artificial neural network to control valves to adjust minor actinide concentration. Such precise control optimizes the most minor actinide burned while remaining safe.

The central tank or chamber <NUM> is a pressurized gas chamber composed of deuterium or tritium gas and functions as the neutron source to ignite the self-sustaining chain reaction in the first and second concentric tanks <NUM> and <NUM>. The first and second tanks <NUM> and <NUM> contain a mixture of FLiBe molten salt and minor actinides. The third concentric tank <NUM> contains fission products that are transmuted into stable or short-lived nuclides. The fourth concentric tank <NUM> is a graphite reflector.

In exemplary embodiments, a mixture of lithium fluoride (LiF) and beryllium fluoride (BeF2) is used as a coolant, a neutron moderator and a solvent of the transuranic elements. The salt mixture is composed of <NUM>:<NUM> ratio of LiF to BeF2, hence the stoichiometric compound is given by Li2BeF4. In the literature, this compound is called FLiBe. The operation of the transmutator in this liquid state is akin to the molten salt reactor (MSR). FLiBe salt has a high heat transfer with capability of carrying the same amount of heat (J/K) as water. The heat capacity of FLiBe is <NUM> J/(kg-K) while water is <NUM> J/(kg-K). Furthermore, the density of FLiBe density is about <NUM> times that of water. FLiBe molten-salt remains liquid up to <NUM>° C without pressurization, providing good safety. For example, a pressure water reactor has an operating temperature of <NUM>° C while being held at <NUM> atmospheres. The FliBe salt solidifies at <NUM>° C, providing good safety in case of accident with loss of coolant.

Fission of TRU elements produces FP (e.g. Tc-<NUM>, <NUM>-<NUM>, Zr-<NUM> are very long lived and Sr-<NUM>, Cs-<NUM> generate almost all radioactivity first <NUM> years). A transmutation [(n,2n), (n,3n) etc.] of FP using fast (> 1MeV) neutron into stable nuclei is also achieved.

The outer most tank <NUM> may be filled with water to control criticality, reactivity and other activities. Further adjustment of criticality may be achieved by replacing the volume of the outer most tank <NUM> with a neutron reflecting boundary such as, e.g., a graphite neutron reflector.

Further adjustment of criticality may be achieved by retaining the outer most tank <NUM> with a volume containing water and surrounding it along the outer radius with a neutron reflecting boundary.

Real-time monitoring of the FLiBe and TRU mixture as well as fission products (FP) in each tank feedbacks the density of TRU and FPs (including real-time injection control of TRU). By adjusting the density of TRU/FLiBe/FP, criticality may be adjusted. Furthermore, with knowledge of the composition of the mixture in a given tank, separation of different FP using solvent extraction techniques is performed.

Between the first concentric tank <NUM> and the second concentric tank <NUM>, a reflector (e.g. beryllium) can be inserted to reflect neutrons back into the first tank <NUM>, and thus increase neutron multiplication. If real-time monitoring determines a certain criticality or other conditions (i.e., temperature, concentration) are satisfied, the pre-programmed feedback control intervenes to retract the reflectors either fully or partially.

Real-time monitoring of the criticality and other physical parameters (i.e., temperature, concentration, and FLiBe chemistry) is performed in all tanks <NUM>, <NUM> and <NUM>, and in any additional tank. Data is then feedback into control circuitry which is connected to valves, pumps etc. to maintain preset parameters.

The neutron generating machine inside the cylindrical tank <NUM> may be positioned on a rail system to easily slide in and out. In one scenario, the machine remains inside the tank <NUM>. In a second scenario, once the real-time monitoring system establishes that a critical value is reached inside the tanks <NUM> and <NUM> with FLiBe/TRU solution, the neutron generator may be withdrawn and reused in a different assembly of tanks <NUM> and <NUM>.

<FIG> shows a partial view of a single assembly of a transmutator <NUM> having a tank <NUM> filled with a mixture of minor actinides and FLiBe and a neutron source tank <NUM> positioned therein. Additional tanks, as shown in <FIG> may enclose the tank <NUM>. In this embodiment, a deuteron beam <NUM> is generated by the electrostatic accelerator <NUM> (see <FIG>) focused by a magnet <NUM> to pass through an entrance port <NUM> to the neutron source tank <NUM>. The energy of the deuteron beam <NUM> is in the range of <NUM>-<NUM> keV (at a current of <NUM> A). The deuteron beam <NUM> then propagates through the pressurized tank <NUM> filled with tritium or deuterium gas. Within the pressurized tank <NUM>, the deuteron beam <NUM> interacts and fuses with tritium or deuterium producing neutrons <NUM>. The neutrons <NUM> are emitted from the pressurized tank <NUM> and interact with and incinerate minor actinides in the concentric tank <NUM>.

<FIG> shows an alternative embodiment of neutron generation with positive deuteron beams. The deuteron beam <NUM> is created and the deuteron beam <NUM> propagates within the neutron source tank <NUM> as described above with regards to the embodiment shown in <FIG>. As depicted in the <FIG>, the deuteron beam <NUM> propagates within the neutron source tank <NUM> onto a solid target <NUM> composed of either titanium-tritium or titanium-deuterium. The deuteron beam <NUM> interacts with either the tritium or deuterium of the solid target <NUM> to generate fusion neutrons <NUM>. The neutrons <NUM> are emitted from the pressurized tank <NUM> and interact with and incinerate minor actinides in the concentric tank <NUM>.

In an alternative embodiment, the solid target <NUM> depicted in <FIG> is composed of titanium. The injected deuteron beam <NUM> imbeds within the titanium lattice, and any subsequent deuteron beams <NUM> then interact with the already imbedded deuterons to create fusion neutrons <NUM>.

<FIG> shows a partial view of an alternative embodiment of a single assembly of a transmutator <NUM> having a tank <NUM> filled with a mixture of minor actinides and FLiBe and a neutron source tank <NUM> positioned therein. A plurality of deuteron beams <NUM> and solid targets <NUM> are provided with the beams <NUM> injected from electrostatic accelerators <NUM> positioned within the neutron source tank <NUM>. A single deuteron beam generator <NUM>, deuteron beam <NUM> and solid target <NUM> are shown in <FIG>. The deuteron beam <NUM> interacts with either the tritium or deuterium solid target <NUM> to generate fusion neutrons <NUM>. The neutrons <NUM> are emitted from the neutron source tank <NUM> and interact with and incinerate minor actinides in the tank <NUM> surrounding the source tank <NUM>.

<FIG> shows a partial view of an alternative embodiment of a single assembly of a transmutator <NUM> having a tank <NUM> filled with a mixture of minor actinides and FLiBe and a neutron source tank <NUM> positioned therein. A plurality of deuteron beam assemblies <NUM> are provided with the beams <NUM> injected external to the neutron source tank <NUM> filled with pressurized tritium or deuterium gas. The deuteron beams <NUM> are injected into the tank <NUM> through the entrance port <NUM> and consequently propagate through the tank <NUM> where the deuteron beams <NUM> interact and fuse with the tritium or deuteron gas to generate neutrons <NUM>. <FIG> shows a single beam assembly <NUM> whereas beam assembly <NUM> and focusing magnet <NUM> are shown. The focused beam <NUM> is subsequently injected into the neutron source tank <NUM> passing through the entrance port <NUM>.

<FIG> shows an alternative embodiment. The plurality of beams <NUM> are injected onto solid targets <NUM> generating fusion neutrons <NUM>. The solid targets <NUM> are composed of either titanium-tritium or titanium-deuterium. The deuteron beam <NUM> interacts with either tritium or deuterium of the solid target <NUM> to generate the fusion neutrons <NUM>. The neutrons <NUM> are emitted from the pressurized tank <NUM> to interact with and incinerate minor actinides in the tank <NUM> surrounding the pressurized tank <NUM>.

Turning to <FIG>, an exemplary embodiment of an electrostatic accelerator beam system is shown. As depicted, a beam system <NUM> is based on positive ion multi-aperture extraction sources and utilizes geometric focusing, inertial cooling of the ion extraction grids and differential pumping. The beam system <NUM> includes an RF plasma source <NUM> at an input end (this can be substituted with an arc source or the like) with a magnetic screen <NUM> covering the end. An ion optical source and acceleration grids <NUM> are coupled to the plasma source <NUM> and a gate valve <NUM> is positioned between the ion optical source and acceleration grids <NUM> and an aiming device <NUM> at the exit end. A cooling system comprises two cryo-refrigerators <NUM>, two cryopanels <NUM> and a LN2 shroud. This flexible design allows for operation over a broad range of parameters.

<FIG> shows a laser operation system <NUM> for the purposes of spectroscopy, active monitoring and fission product separation. Component A is the CAN laser (in bundles appropriately); component B is the modulator /controller of the CAN laser (controlling the laser properties such as the power level, amplitude shape, periods and phases, the relative operations, direction, etc.); component C is the laser rays irradiating the solution and solvents in the central tank (see component K) for both the monitoring and separation (or controlling the chemistry of the solvents); component D is the solution that contains solvents including the transuraniums (such as Am, Cm, Np) ions that are to be separated and transmuted by the transmutator E [Ref. <NUM>] (emanating fusion produced high energy neutrons); component F is the water that stops the neutrons both from the fusion source, i.e., transmutator E, and from the fission products; component G is the precipitation that is to be taken out of the deposit at the bottom of the central tank (as an example of a separation by laser chemistry in the central tank where solution is contained); component H is the unnecessary deposited elements that are not to be transmuted at this time in this particular tank and to be transferred to another tank, where they will be again in the solution similar to this to be further separated and transmuted; component I is the feedback ANN circuit and computer that registers and controls the signal of the monitored information such as spectrum of the FP; component J is the detector of the transmitted CAN laser signals (amplitudes, phases and frequencies, and deflections, etc.); component K is the "thin" first wall of the central tank that allow nearly free transmission of the energetic neutrons generated either by fusion or fission in the central tank, and component L is the outer tank with a thick enough wall that contains overall materials and neutrons. Both the central tank K and the outer tank L are equipped with appropriate monitors of the temperature, pressure, and some additional physical and chemical information in addition to the CAN laser monitoring to monitor, and provide alerts regarding, the transmutator's condition to keep the tanks from going over the "board" (such as runaway events) with appropriate safeguards such as the real-timed valves, electrical switches, etc. Component Q is a heat exchanger and component M converts heat to electricity.

Once the operation begins, the heated solution and water in the central and outer tanks K and L may be maintained in its state by motors (or perhaps appropriate channels inside the tanks, or equivalents) as desired, and excess heat is taken out and converted into electrical (or chemical) energies by component M.

Referring to <FIG>, in a system <NUM>, component P is the pipe (and its valve that controls the flow between the tanks) connecting the segregated separator tank and the transmutator tank. Component O is a solving region of the injected separated MA into the transmutator tank. The residual fission products left in component D are transported out through the pipe component R into a storage tank component S.

Referring to <FIG>, in a system <NUM>, the central tank K contains the solution D of the transuraniums that were extracted from the original spent fuel that has been liquefied with proper solutions (such as acids). In this stage of the process, we assume that U and Pu have been already extracted from the solution D by known processes (such as PUREX). The solution D may thus include other elements such as fission products (FPs such as Cs, Sr, I, Zr, Tc, etc.). These elements can tend to absorb neutrons, but not necessarily proliferate neutrons as the transuraniums tend to do. Thus, the FPs need to be eliminated from the solution D in the central tank K by chemical reactions and laser chemistry, etc., with the help of the CAN laser A and other chemical means. If these elements precipitate by the added chemical and/or chemical excitation etc. from the CAN laser, the precipitated components of chemicals may be removed from this central tank K to another tank for the treatment of such elements as the fission products etc..

Upon completion of the separation process, the transuraniums (mainly Am, Cm, Np) are irradiated with neutrons from the transmutator E. These transuraniums may have different isotopes, but all of them are radioactive isotopes, as they are beyond uranium in their atomic number. Either neutrons from the transmutator E or neutrons arising from the fissions of the transuraniums will contribute to the transmutation of the transuraniums if neutrons are absorbed by these nuclei.

Turning to <FIG>, the transmutator and laser monitor and separator system <NUM> includes two separate tanks segregating the separation and transmutation processes into two distinct tanks. For example, the separator (with laser monitor attached) is on the right, while the transmutator is on the left. The two systems are connected by a transmission pipe and valve, component P, which is used to transmit the deposited (or separated) transuraniums (MA) from the separator tank on the right into the transmutator tank on the left. The new carrier liquid (component O) preferably only contains (or primarily contains) TA, but not any more fission products that have been separated in the separator tank on the right. Separation is accomplished by either conventional chemical method or by laser (based on CAN laser), which operates to excite (for example) the MA atomic electrons for the purpose of chemical separation. The central tank D on the left has primarily (or only) MA solution. The elements left out of the liquid contain mainly FPs that are transported in a pipe (component R) into a storage tank (component S). Such FPs may be put together into solidified materials for burial treatment. <NUM> and <NUM>].

When fission occurs by the neutron capture by the transuraniums, a high-energy yield from the nuclear fission is typically expected (such as in the range of 200MeV per fission). On the other hand, the fusion neutron energy does not exceed 15MeV. Both the fusion neutrons as well as the fission events in the central tank yield heat in the tank. The solution mixes the heat in general by the convective flows (either by itself or, if necessary, by an externally driven motor). The extracted heat transporter and extractor, i.e. component M, remove the generated heat in the central tank and convert it into electric energy. These processes need to be monitored both physically (such as the temperature, pressure of the solution in the tank) and chemically (such as the chemical states of various molecules, atoms, and ions in the solution through the CAN laser monitoring) in real time for the monitoring and control purpose to feedback to the tank parameters by controlling valves and other knobs as well as the CAN operation.

A typical nuclear reactor generates the following spent fuel nuclear wastes. <NUM> and <NUM>] Per <NUM> ton of uranium which generates 50GWd of power. During this operation the nuclear wastes are: about <NUM> of transuraniums (Np, Am, Cm) and about <NUM> of fission products. The amount of <NUM> of MA (Minor Actinides, i.e. transuraniums) is about 100mol, approximately <NUM> x <NUM> atoms of MA. This amounts to about <NUM> x <NUM> atoms of MA per second, approximately <NUM> MA atoms in <NUM> sec. This translates into about 1kW of laser power if the absorption of one photon (eV) by each MA atom in order to laser excite each atom is required. Let η be the efficiency of excitation of an MA atom by <NUM> photon of laser. Then the power P of the laser to be absorbed by all MA atoms of the above amount per second is <MAT>.

If η ∼ <NUM>, P is about 100kW. This amount is not small. On the other hand, borrowing efficient and large fluence CAN laser technology [Ref. <NUM>], it is within the realm of the technology reach. In typical chemical inducements, we envision that the laser may be either close to cw, or very long pulse so that the fiber laser efficiency and fluence are at its maximum. In order to satisfy the proper resonances or specific frequencies, the fiber laser frequencies need to be tuned (prior to the operation, most likely) to the specific values.

As further exemplary embodiments, the high efficiency neutron generation method is applicable to fields and processes requiring neutrons having energy up to <NUM> MeV, such as, e.g., cancer medical applications such as, e.g., boron-neutron capture therapy (BNCT) and radioisotope generation, structural integrity testing of buildings, bridges, etc., material science and chip testing, oil well logging and the like.

Two additional embodiments are presented: (<NUM>) a first embodiment directed to a <NUM>-tank strategy to reduce the overall neutron cost whereas Tank <NUM> is critical and Tank <NUM> subcritical, and (<NUM>) second embodiment directed toward a greener, carbon negative trasmutator through the generation of synthetic fuel by the chemical conversion of CO_2 whereas the heat to drive the reaction is generated by fission.

In an example embodiment depicted in <FIG>, the transmutator <NUM> comprises two interconnected sets of tanks referred to as Tank <NUM> and Tank <NUM>. Tanks <NUM> and <NUM>, which are substantially similar to the tanks depicted in Figures 2A and 3A, may include a tank containing materials to be transmuted and a neutron source tank positioned therein, and as depicted in <FIG>, these tanks may be enclosed by additional concentric tanks. Tank <NUM> preferably contains a mixture of Pu and minor actinides (MA) including neptunium, americium and curium (Np, Am, Cm), while Tank <NUM> contains a mixture of only minor actinides (MA). Tank <NUM> is critical (keff = <NUM>), hence Tank <NUM> does not require external neutrons. Furthermore, Tank <NUM> is fueled using the spent nuclear fuel (Pu and MA) after chemical removal of fission products. Tank <NUM> utilizes fast neutrons (fusion neutrons in addition to unmoderated fission neutrons with energy ><NUM> MeV) to transmute the minor actinides (MA) and plutonium (Pu), while the concentration of curium (Cm) is increased. Alternatively, a minor amount of neutrons can be injected into Tank <NUM> to kick start the incineration of Pu.

The minor actinides (MA) in Tank <NUM>, now with higher concentration of curium (Cm), may be separated and fed into Tank <NUM>. The connected Tank <NUM> operates in parallel to burn the minor actinides (MA) with the increased concentration of curium (Cm) in a subcritical (keff < <NUM>) operation, as described above. This process provides a path to safely and smoothly burn the entire transuranic spent nuclear fuel (not just MAs) while reducing the number of neutrons required to do so by about a factor of 100x.

In a further embodiment, Tank <NUM> and Tank <NUM> are real-time monitored by laser and gamma. A broadband or a scanning laser is used to monitor the elemental composition of Tank <NUM> and Tank <NUM> using the laser induced fluorescence and scattering. Gamma monitoring can be either active or passive. Passive gamma monitoring utilizes gamma generated from nuclear decay or transition. Active gamma monitoring utilizes external gamma beam with energy above few MeV and relies on the nuclear resonance fluorescence. Both active and passive monitoring provides information about the isotopic composition of the transmutator fuel. Information from the laser and the gamma monitoring is collected and fed into a computer comprising logic adapted to predict and/or control future states of the transmutator by adjusting the refueling of Tank <NUM> or adjusting the MA concentration in Tank <NUM>. To enable the detailed laser and gamma monitoring the fuel in Tank <NUM> and Tank <NUM> is dissolved in a molten salt allowing for light propagation. Real time monitoring is an integral part of the overall active safety and efficiency of the transmutator whereas a detail knowledge of the transmutator composition will determine the position of the control rods, the refueling and fission product extraction. Passive features include molten salt that expands with increasing temperature thus shutting the transmutator down; dump tank separated from the transmutator by a freeze plug whereas any abnormal temperature spike will melt the plug and gravity flow the entire inventory of the transmutator into the dump tank composed of neutron absorbers.

The walls of Tank <NUM> and Tank <NUM> are made of diamond. To protect walls from chemical erosion and corrosion, the salt adjacent to the wall (facing the molten salt) is allowed to solidify preventing direct contact of the molten salt with the walls.

In a further embodiment, the transmutator embodiments described above can be applied to the methods and processes of carbon dioxide reduction such as its use as a coolant and its generation of a synthetic fuel to become overall carbon-negative is suggested. In the following example embodiment, the synthetic fuel (CH<NUM> - methane) may be generated via CO<NUM> + <NUM>H<NUM> → CH<NUM> + <NUM>H<NUM>O reaction (Sabatier reaction) requiring <NUM>-<NUM> and the presence of a catalyst, e.g., Ni, Cu, Ru. The CO<NUM> may be extracted from the atmosphere, the ocean, or by direct capturing of CO<NUM> at the source of emission such as automobiles, houses, chimneys and smokestacks. The molten salt transmutator operating temperature range is <NUM> -<NUM> and, thus, is ideally situated to supply continuously the necessary temperature required to drive the Sabatier reaction to produce methane, and provide an effective pathway to stabilize and reduce the CO<NUM> concentration in the atmosphere and the ocean.

Referring to <FIG>, a partial view of a synthetic fuel generation system <NUM> is shown to include a transmutator vessel <NUM>, a secondary loop pipe <NUM>, the direction of the flow of the molten salt + TRU <NUM>, a heat exchanger <NUM>, and a tank for the Sabatier reaction <NUM>. In this example embodiment, the heat transfer fluid in the heat exchanger pipe is CO2 which is directly used in the tank <NUM>. In an alternative embodiment, shown in <FIG>, the heat exchange pipe of the heat exchanger <NUM> of a synthetic fuel generation system <NUM> is a closed and independent system, and the transfer fluid may be replaced with a molten salt. The synthetic fuel generation system <NUM> is shown to include a transmutator vessel <NUM>, a secondary loop pipe <NUM>, the direction of the flow of the molten salt + TRU <NUM>, a heat exchanger <NUM>, and a tank for the Sabatier reaction <NUM>.

In a further alternative embodiment, <FIG> shows a partial view of a synthetic fuel generation system <NUM> having a transmutator <NUM>, a heat exchanger <NUM>, the direction of the flow of the fluid <NUM>, and a tank for the Sabatier reaction <NUM>. In this example embodiment, the reactant, CO<NUM>, from the Sabatier reaction is the transfer fluid. In an alternative embodiment, <FIG> shows the heat exchanger loop <NUM> of a synthetic fuel generation system <NUM> as closed and independent loop with the heat transfer fluid being, for example, a molten salt. The synthetic fuel generation system <NUM> is shown to include a transmutator <NUM>, a heat exchanger <NUM>, the direction of the flow of the fluid <NUM>, and a tank for the Sabatier reaction <NUM>.

In an additional embodiment, ionizing radiation originating within the transmutator and carried by the molten salt is utilized as a <NUM>-<NUM> eV energy source to enable various chemical reactions. The <NUM>-<NUM> eV energy source enables, for example, the production of ammonia and conversion of CO_2+CH_4→CH_3 COOH.

Processing circuitry for use with embodiments of the present disclosure can include one or more computers, processors, microprocessors, controllers, and/or microcontrollers, each of which can be a discrete chip or distributed amongst (and a portion of) a number of different chips. Processing circuitry for use with embodiments of the present disclosure can include a digital signal processor, which can be implemented in hardware and/or software of the processing circuitry for use with embodiments of the present disclosure. In some embodiments, a DSP is a discrete semiconductor chip. Processing circuitry for use with embodiments of the present disclosure can be communicatively coupled with the other components of the figures herein. Processing circuitry for use with embodiments of the present disclosure can execute software instructions stored on memory that cause the processing circuitry to take a host of different actions and control the other components in figures herein.

Processing circuitry for use with embodiments of the present disclosure can also perform other software and/or hardware routines. For example, processing circuitry for use with embodiments of the present disclosure can interface with communication circuitry and perform analog-to-digital conversions, encoding and decoding, other digital signal processing and other functions that facilitate the conversion of voice, video, and data signals into a format (e.g., in-phase and quadrature) suitable for provision to communication circuitry, and can cause communication circuitry to transmit the RF signals wirelessly over links.

Communication circuitry for use with embodiments of the present disclosure can be implemented as one or more chips and/or components (e.g., transmitter, receiver, transceiver, and/or other communication circuitry) that perform wireless communications over links under the appropriate protocol (e.g., Wi-Fi, Bluetooth, Bluetooth Low Energy, Near Field Communication (NFC), Radio Frequency Identification (RFID), proprietary protocols, and others. One or more other antennas can be included with communication circuitry as needed to operate with the various protocols and circuits. In some embodiments, communication circuitry for use with embodiments of the present disclosure can share an antenna for transmission over links. Processing circuitry for use with embodiments of the present disclosure can also interface with communication circuitry to perform the reverse functions necessary to receive a wireless transmission and convert it into digital data, voice, and video. RF communication circuitry can include a transmitter and a receiver (e.g., integrated as a transceiver) and associated encoder logic. A reader can also include communication circuitry and interfaces for wired communication (e.g., a USB port, etc.) as well as circuitry for determining the geographic position of reader device (e.g., global positioning system (GPS) hardware).

Processing circuitry for use with embodiments of the present disclosure can also be adapted to execute the operating system and any software applications that reside on a reader device, process video and graphics, and perform those other functions not related to the processing of communications transmitted and received. Any number of applications (also known as "user interface applications") can be executed by processing circuitry on a dedicated or mobile phone reader device at any one time, and may include one or more applications that are related to a diabetes monitoring regime, in addition to the other commonly used applications, e.g., smart phone apps that are unrelated to such a regime like email, calendar, weather, sports, games, etc..

Memory for use with embodiments of the present disclosure can be shared by one or more of the various functional units present within a reader device, or can be distributed amongst two or more of them (e.g., as separate memories present within different chips). Memory can also be a separate chip of its own. Memory can be non-transitory, and can be volatile (e.g., RAM, etc.) and/or non-volatile memory (e.g., ROM, flash memory, F-RAM, etc.).

Computer program instructions for carrying out operations in accordance with the described subject matter may be written in any combination of one or more programming languages, including an object oriented programming language such as Java, JavaScript, Smalltalk, C++, C#, Transact-SQL, XML, PHP or the like and conventional procedural programming languages, such as the "C" programming language or similar programming languages. The program instructions may execute entirely on the user's computing device (e.g., reader) or partly on the user's computing device. The program instructions may reside partly on the user's computing device and partly on a remote computing device or entirely on the remote computing device or server, e.g., for instances where the identified frequency is uploaded to the remote location for processing. In the latter scenario, the remote computing device may be connected to the user's computing device through any type of network, or the connection may be made to an external computer.

To the extent the embodiments disclosed herein include or operate in association with memory, storage, and/or computer readable media, then that memory, storage, and/or computer readable media are non-transitory. Accordingly, to the extent that memory, storage, and/or computer readable media are covered by one or more claims, then that memory, storage, and/or computer readable media is only non-transitory.

Claim 1:
A transmutator system (<NUM>) for transmutation of long-lived radioactive transuranic waste comprising:
a neutron source tank (<NUM>) including a neutron source therein,
a plurality of concentric tanks (<NUM>,<NUM>) positioned about the neutron source tank and comprising a one or more mixtures of long-lived radioactive transuranic waste dissolved in FLiBe salt; characterised in that the system further comprises:
an electrostatic accelerator (<NUM>) oriented to axially propagate a deuteron beam into the neutron source,
characterised in that
the plurality of concentric tanks form a first set of tanks and wherein the transmutator system further comprising a second set of tanks containing a mixture of Pu and minor actinides including neptunium, americium and curium and wherein the walls of one of the first set of tanks or the second set of tanks are made of carbon based materials and wherein the carbon based materials are diamond.