This application is related to the US patent application entitled “Pressure Wave Generator and Controller for Generating a Pressure Wave in a Fusion Reactor” by Laberge et al. filed concurrently herewith and incorporated herein by reference.
1. Field of Invention
This invention relates to fusionable material targets for use in fusion reactors.
2. Description of Related Art
Nuclear fusion reactions involve bringing together atomic nuclei against their mutual electrostatic repulsion and fusing them together to make heavier nuclei, while at the same time releasing energy. Isotopes of light elements (i.e. elements having a relatively small number of protons) are the easiest to fuse, because the electrostatic repulsion between the nuclei of light elements is smaller than that of heavier elements. The use of light elements may produce significantly reduced collateral radioactivity than comparable fission reactors, which typically use isotopes of heavier elements.
Inducing nuclear fusion reactions is difficult, because of the energies required to accelerate the nuclei to speeds fast enough to overcome their mutual electrostatic repulsion and because the nuclei are so small that the chance that two passing nuclei will interact with one another in a manner which results in fusion of the nuclei is small.
Fusion reactors typically require input energy to initiate fusion reactions. The amount of input energy required is largely determined by the need to accelerate the nuclear reactants to thermonuclear speed and to confine the nuclear reactants in a space that allows them to interact. A reactor that consumes less energy than it produces is said to produce net energy. Such a reactor will have an efficiency ratio (the ratio of energy output to the energy input) greater that unity. The energy output of a fusion reactor is largely determined by the number of fusion reactions that are induced in the reactor and the amount of energy that is released and captured.
There remains a need for methods and apparatus that facilitate improvements to the efficiency of nuclear fusion reactors.
In accordance with one aspect of the invention there is provided in a fusion reactor having fusion reactions initiated by a pressure wave in a heated liquid medium, a method for confining a fusionable material in a fusionable material target. The method involves enclosing fusionable material in a container operable to be cooled until at least some of the fusionable material is in a solidified state. The container is operable to be received in the heated liquid medium. The method also involves heat insulating the container while the container is in the heated liquid medium for a time sufficient to maintain at least some of the fusionable material in the solidified state until fusion is initiated by the pressure wave.
Enclosing fusionable material in the container comprises enclosing fusionable material in a glass micro-balloon.
Enclosing fusionable material in the container may involve diffusing fusionable material into the container.
Insulating the container may involve enclosing the container in a metal shell.
Enclosing the container in the metal shell may involve enclosing the container in a lead and lithium shell.
The method may involve grading a density of the metal shell such that the density increases from an inner surface of the shell to an outer surface of the shell.
Enclosing fusionable material in a container may involve enclosing fusionable material in a first container and may further involve enclosing the first container in a second container and evacuating a space between the first container and the second container.
The method may involve holding the first container in the second container.
The method may involve forming a reflective coating on an outside surface of the first container.
In accordance with another aspect of the invention there is provided a fusionable material target apparatus for use in a fusion reactor having fusion reactions initiated by a pressure wave in a heated liquid medium. The apparatus includes provisions for enclosing fusionable material in a container operable to be cooled until at least some of the fusionable material is in a solidified state, the container operable to be received in the heated liquid medium. The apparatus also includes provisions for heat insulating the container while the container is in the heated liquid medium for a time sufficient to maintain at least some of the fusionable material in the solidified state until fusion is initiated by the pressure wave.
In accordance with another aspect of the invention there is provided a fusionable material target apparatus for use in a fusion reactor having fusion reactions initiated by a pressure wave in a heated liquid medium. The apparatus includes a container for enclosing fusionable material, the container being operable to be cooled until at least some of the fusionable material is in a solidified state. The container operable to be received in the heated liquid medium. The apparatus also includes a heat insulator for insulating the container while the container is in the heated liquid medium for a time sufficient to maintain at least some of the fusionable material in the solidified state until fusion is initiated by the pressure wave.
The container may include a glass micro-balloon.
The container may include a metal shell.
The metal shell may include a lead and lithium shell.
The insulator may include a metal shell having a graded density such that the density increases from an inner surface of the metal shell to an outer surface of the metal shell.
The container may include a first container and the heat insulator may include a second container. The second container may be operably configured to enclose the first container such that a space is formed between the first container and the second container, the space being evacuated.
The apparatus may include a pair of wires for holding the first container in the second container.
The apparatus may include a reflective coating formed on an outside surface of the first container.
In accordance with another aspect of the invention there is provided a fusionable material target apparatus for use in a fusion reactor comprising a container for enclosing fusionable material, the container having a wall formed of lithium salt.
Other aspects and features of the present invention will become apparent to those ordinarily skilled in the art upon review of the following description of specific embodiments of the invention in conjunction with the accompanying figures.
In drawings which illustrate embodiments of the invention,
Referring to
The wall 108 of the fusion reactor 100 further includes an inlet aperture 120 and an outlet aperture 122 disposed on diametrically opposite sides of the reactor. The fusion reactor 100 also includes an inlet conduit 124 in communication with the inlet aperture 120 and an outlet conduit 126 in communication with the outlet aperture 122. The fusion reactor 100 further includes a recirculation system 128, which includes an input 130 in communication with the outlet conduit 126 and an output 132 in communication with the inlet conduit 124. The recirculation system 128 also includes a pump (not shown) for circulating the liquid medium 118 through the fusion reactor 100 and may also include facilities for maintaining the liquid medium at a desired temperature by adding or extracting heat energy from the liquid medium. The recirculation system 128 may also include a turbine (not shown) for converting heat energy into electrical energy.
The pressure wave generators 104 are located on the outside surface 112 of the wall 108 (only some of the pressure wave generators are shown for clarity). Each pressure wave generator 104 includes a housing 140 and a piston 142, which is moveable in the housing and capable of impacting the outside surface 112 of the wall 108 to cause a pressure wave to be generated in the liquid medium 118. Each pressure wave generator 104 further includes a fluid port 146, in communication with a source of pressurised fluid (not shown), for applying a fluid pressure to the housing 140 to actuate the piston 142. Each pressure wave generator 104 may be independently controllable, allowing respective pistons to impact the outside surface 112 of the wall 108 at a desired time and with a desired amount of kinetic energy. The kinetic energy due to the piston impact causes a compression wave in the wall 108 which travels through the wall and into the liquid medium 118, thus generating a pressure wave in the liquid medium. In some embodiments the wall 108 may include a moveable transducer 144 in the wall 108 (only one moveable transducer is shown in
The fusion reactor 100 also includes a reservoir 134, in communication with the inlet conduit 124 through a valve 138. The reservoir 134 holds fusionable material targets 136 and, in combination with the valve 138, facilitates the introduction of the fusionable material targets 136 into the liquid medium 118 through the inlet conduit 124. The fusionable material target 136 may include fusionable material in a gaseous form and may include an isotope of a light element, such as deuterium, tritium, 3He, or a combination thereof. The fusion reactor 100 also includes a Dewar 148 for containing a liquefied gas 150. The Dewar 148 encloses the reservoir 134, facilitating cooling of the fusionable material targets 136 by liquefied gasses, such as Helium or Nitrogen, to very low temperatures.
The fusionable material target 136 is shown in greater detail in
The operation of the fusionable material target 136 is described with reference to
The valve 138 is then activated to allow one of the fusionable material targets 136 to be introduced into the inlet conduit 124 from the reservoir 134. The recirculation system 128 causes a flow of the liquid medium 118 into the inner cavity 114 in a direction shown by arrow 152. The fusionable material target 136 is carried upwardly into the inner cavity 114 by the buoyancy of the target and the flow in the direction 152. When the fusionable material target 136 reaches a point in the inner cavity 114 that is proximate a center 137 of the inner cavity, a pressure wave is initiated in the liquid medium 118. Since the upwards movement of the fusionable material target 136 continues while the pressure wave propagates through the liquid medium 118, the activation of the pistons 142 is timed such that the pressure wave converges to the location of the target when the target reaches the center 137 of the inner cavity 114. A suitable controller for timing the initiation of the pressure wave is described in the related application “Pressure Wave Generator and Controller for Generating a Pressure Wave in a Fusion Reactor” by Laberge et al.
The liquid medium 118 may include a mixture of molten metals such as lead or lithium and the temperature of the liquid medium may be 400 degrees Celsius or greater. When the fusionable material target 136 is introduced into the liquid medium 118, the heat insulating metal 183 will begin to melt. However, the composition and thickness of insulating metal 183 is selected such that the solidified fusionable material layer 186 remains at least partially frozen while the fusionable material target 136 moves towards the center 137 of the inner cavity 114. Consequently, the container 182 is at least partially insulated from the hot liquid medium 118 by the insulating metal 183, thus facilitating introduction of the target into the fusion reactor such that at least a portion of the solidified fusionable material layer 186 will remain frozen.
As previously described, the pressure wave is initiated such that it converges on the fusionable material target 136 when the target reaches the center 137 of the inner cavity 114. The pressure wave has a pressure wavefront 154 that envelopes and converges on the fusionable material target 136. Referring to
The gaseous fusionable material 191 heats up much quicker than the solidified fusionable material layer 186 and thus fusion reactions will be initiated in the gaseous fusionable material before the solidified fusionable material layer completely melts. The fusion reaction in the gaseous fusionable material 190 generates neutrons and alpha particles. For a fusionable material of deuterium-tritium (D-T), approximately 20% of the fusion energy will be released in the form of fast alpha particles. These alpha particles have a very short range and will therefore deposit a substantial portion of their energy in the solidified fusionable material layer 186, thus heating up this layer. This heating in turn initiates further fusion reactions which generate further alpha particles thus causing a detonation front to propagate in the fusionable material target 136.
In contrast, for a fusionable material target that has all the fusionable material in the gaseous form, it is necessary to heat and compress a larger amount of fusionable material all at once. Additional energy is required to confine the fusionable materials while heating the materials to fusion temperatures. Thus for a purely gaseous fusionable material, additional energy is required in the pressure wave to both heat and confine the fusionable materials. Advantageously, the fusionable material target 136 requires less input energy in the form of a pressure wave to initiate fusion reactions since the pressure wave energy is initially concentrated on the gaseous fusionable material 191, which is a smaller quantity than the solidified fusionable material layer of fusionable materials.
A method for fabricating the fusionable material target 136 is described with reference to
Referring to
Referring to
Referring to
As described above in relation to other embodiments, the fusionable material target may be cooled such that at least a portion of the gaseous fusionable material 258 solidifies. The evacuated space 260 operates as a very good insulator of heat. When the target is to be introduced into a fusion reactor having a hot liquid medium 118, the evacuated space 260 and the reflective layer 268 insulate the fusionable material, such that the frozen fusionable materials remain at least partially frozen. The use of the reflective layer 268 further improves the insulation by reflecting energy having infrared wavelengths, thus further insulating the solidified fusionable material layer 258.
Referring to
While specific embodiments of the invention have been described and illustrated, such embodiments should be considered illustrative of the invention only and not as limiting the invention as construed in accordance with the accompanying claims.