The present invention relates to a nuclear reactor.
Nuclear reactors are used for electric power generating facilities. Nuclear reactors include fast neutron reactors. Fast neutron reactor are nuclear reactors which mainly use fast neutrons to cause fission of fissionable nuclides to generate output. Sodium, lead-bismuth alloys, and other heavy metals and, further, gas are used to cool the core. In nuclear reactors of the prior art, fission occurs at the core as a whole to generate output.
The criticality of the core of a nuclear reactor is maintained and the output is adjusted by for example control rods. The control rods are formed by a material which easily absorbs neutrons. At the start of a burning cycle, control rods are inserted into the core, and the control rods are gradually withdrawn along with the progress in burning so as to maintain the critical state while maintaining output. In this way, in operation of a nuclear reactor, control is necessary for maintaining the criticality of the nuclear reactor. Control is performed for maintaining the criticality on a continuous basis from the start of the burning cycle to the end of the burning cycle.
Japanese Patent No. 3463100 discloses a nuclear reactor in which control for maintaining the criticality in the burning cycle is unnecessary. This nuclear reactor employs the burning method called CANDLE (Constant Axial Shape of Neutron Flux, Nuclide Densities and Power Shape During Life of Energy Production) burning. In CANDLE burning, the core can be divided into a generally new fuel part, burning part, and burned up part. The burning part moves toward the new fuel part by a speed proportional to output along with burning. In CANDLE burning, after a single burning cycle is ended, fuel is replaced for the next burning cycle. When replacing the fuel, the burned up fuel can be taken out in the core axial direction and new fuel can be loaded in the end at the opposite side to the end at the taken out side.
In CANDLE burning, there is no need for adjustment of criticality. Further, even if not adjusting the power density distribution, the power density distribution is maintained substantially constant. For this reason, there is the feature that from the beginning to the end of the burning cycle, there is no need for control of the reactivity of the core such as manipulation of the control rods. Further, there is the feature that the reactivity coefficient does not change and it is not necessary to change the method of operation together with burning.
PLT 1: Japanese Patent No. 3463100
By employing CANDLE burning as the method of burning fuel at a nuclear reactor, it is possible to provide a nuclear reactor in which the core properties can be maintained substantially constant even when burning progresses, control of the operation becomes simple, and the probability of accidents is low. Further, there is no need to arrange control rods in the core, so there is no possibility of accidents where the control rods are mistakenly pulled out during the operating period. Further, the burnup when taking out the fuel is high, so it is possible to reduce the amount of waste.
In CANDLE burning, as the new fuel for the second cycle and on, it is possible to use natural uranium or depleted uranium alone for operation. These fuels are subcritical, so are easy to transport and store. Further, it is possible to utilize about 40% of the uranium as energy without enrichment or reprocessing, so resources can be effectively utilized. Further, since the new fuel of the second cycle and on does not require enrichment, reprocessing, etc., there is the feature of a high proliferation resistance.
In this regard, in the conventional art, a nuclear reactor is started and stopped by using control rods. For example, during operation of a nuclear reactor, control rods can be inserted into the core so as to lower the power of the nuclear reactor and cause it to stop. Further, at the time of startup of a nuclear reactor, the inserted control rods can be pulled out to make the core critical, then raise the power of the core.
Even in a nuclear reactor which is provided with a core which employs CANDLE burning, it is possible to arrange control rods which are inserted into the core so as to start and stop the nuclear reactor. However, in CANDLE burning, if forming the channels for insertion of the control rods in the core, reaching criticality sometimes becomes difficult. In cores in the conventional art, it was possible to increase the concentration of fissionable uranium or the concentration of plutonium or increase the number of fuel assemblies of new fuel so as to reach criticality. In CANDLE burning as well, enriched uranium etc. can be included in the new fuel, but it is preferable not to use enriched uranium and to use only natural uranium or depleted uranium as new fuel.
Further, to make the fuel uniformly burn, it is preferable that the power density distribution in the radial direction be substantially constant. In this regard, if forming channels for insertion of control rods at the core, spaces will be formed in the core where no fuel is charged. In these spaces, the power density will end up becoming smaller and therefore there will be the problem that the power density distribution in the radial direction will become uneven.
The present invention has as its object the provision of a nuclear reactor which is provided with a core in which a burning part moves toward a new fuel part along with burning of fuel and which can be started and stopped even without provision of control rods.
The nuclear reactor of the present invention is a nuclear reactor which is provided with a core which includes a new fuel part at which new fuel is loaded and a burning part which is arranged at one side of the new fuel part and which generates neutrons to enable the fuel to burn, the new fuel includes at least one type of uranium from among natural uranium and depleted uranium, the uranium absorbs neutrons to generate plutonium which fissions to generate power, and the burning part moves in a direction toward the new fuel part from the beginning to end of the burning cycle. During the period of power operation, a plurality of fuel assemblies are arranged at the core. The plurality of fuel assemblies include fuel assemblies which are fastened to the core and fuel assemblies which can move in the axial direction of the core. The movable fuel assemblies are pulled out from the core so as to make the nuclear reactor stop and the movable fuel assemblies are inserted into the core from the pulled out state so as to start the nuclear reactor.
In the present invention, preferably the reactor is provided with auxiliary members which include an absorption substance which absorbs neutrons, the auxiliary members are coupled with the movable fuel assemblies, and, when stopping the nuclear reactor, the auxiliary members are inserted into the core along with the movable fuel assemblies being pulled out from the core.
In the present invention, preferably the movable fuel assemblies are formed so that the fuel assemblies as a whole are pulled out from the core.
In the present invention, the core may be divided into a center region and a peripheral region, the movable fuel assemblies may be arranged in the center region, and the fuel assemblies which are fastened to the core may be arranged at the peripheral region.
In the present invention, the movable fuel assemblies may be arranged at the core while separated at predetermined intervals.
According to the present invention, it is possible to provide a nuclear reactor which is provided with a core in which a burning part moves toward a new fuel part along with burning of fuel and which can be started and stopped even without provision of control rods.
Referring to
The coolant, as shown by the arrow 112, flows into the reactor vessel 9 and passes through the inside of the core 10. The heat of the core 10 is transmitted to the coolant. In the nuclear reactor 1 in the present embodiment, the coolant flows from the bottom side to the top side of the core 10. The coolant which flows out from the core 10 flows out from the reactor vessel 9 as shown by the arrow 111.
For the coolant, it is possible to use a material with a small neutron moderating ability and a small neutron absorption ability. In the present embodiment, a lead-bismuth coolant is used. In the present embodiment, the coolant has the function of a reflecting material. As the coolant of the nuclear reactor, in addition to a lead-based coolant (liquid metal), it is possible to use sodium. Further, it is possible to use helium or another gas coolant. Further, as the lead-based coolant, it is possible to employ lead alone in addition to lead-bismuth or the separated isotope lead 208.
Referring to
The core 10 in the present embodiment is divided into a center region and a peripheral region when seen by a plan view. The core in the present embodiment 10 includes a plurality of fuel assemblies. The core 10 of the nuclear reactor in the present embodiment has the fuel assemblies arranged regularly. At the peripheral region of the core, first fuel assemblies comprised of fuel assemblies 21a are arranged. At the center region of the core, second fuel assemblies comprised of fuel assemblies 21b are arranged.
The fuel assemblies 21a and the fuel assemblies 21b in the present embodiment are loaded with the same new fuel. In the present embodiment, depleted uranium is loaded. Further, the fuel assemblies 21a and the fuel assemblies 21b have substantially the same structures for supporting the fuel. The fuel assemblies 21a and the fuel assemblies 21b in the present embodiment are formed so as to be the same heights as each other. The fuel assemblies 21a which are arranged at the peripheral region are fastened to the core 10. On the other hand, the fuel assemblies 21b which are arranged at the center region are formed to be able to move in the axial direction of the core as explained later. In the core in the present embodiment, the vertical direction corresponds to the axial direction of the core.
Each first fuel assembly 21a includes a plurality of fuel rods 22a. The fuel rods 22a are supported by nozzles 27 at their longitudinal direction ends. The fuel rods 22a are supported by a plurality of support grids 25. The nozzles 27 and the support grids 25 support the fuel rods 22a to be separated from each other. In the present embodiment, the support grids are used to maintain the distance between the fuel rods, but the invention is not limited to this. Instead of support grids, it is also possible to use wire spacers etc. The coolant flows between the fuel rods 22a and cools the fuel rods 22a.
The fuel rod shown in
In this way, in the fuel rod 22a in the present embodiment, fuel pellets 24aa, 24ab, 24ac of different burnup are arranged. After the end of one burning cycle, for example, the cladding material 23a is stripped off and the fuel pellets of the burned up part and the other fuel pellets are separated. Next, fuel pellets containing new fuel and the recovered fuel pellets are arranged inside a new cladding material, whereby it is possible to form a fuel rod for the next burning cycle.
Further, as the method of recovering fuel pellets, it is also possible to cut the fuel rod at each part, then strip off the cladding material 23a. This method may also be used to recover fuel pellets which were arranged at the burning part and burned up part.
Referring to
Referring to
Each auxiliary member 51 includes a plurality of absorption rods 52. The absorption rods 52 have cladding materials and have absorption substances arranged inside the cladding materials. The auxiliary member 51 has support grids 25 and nozzles 27 for supporting the absorption rods 52. These support grids 25 and nozzles 27 may be ones similar to those used for the fuel assemblies 21a, 21b.
Each auxiliary member 51 is coupled with a fuel assembly 21b. The fuel assembly 21b includes a plurality of fuel rods 22b. In the present embodiment, a fuel assembly 21b is coupled with an auxiliary member 51 through a coupling member 61. The fuel assembly 21b is connected to the auxiliary member 51 in line in the axial direction of the core.
Referring to
Next, the power operation of the core in the present embodiment will be explained. In the present embodiment, an example where the power is maintained substantially constant during the power operation will be explained.
The core 10 of the nuclear reactor in the present embodiment is one in which the burning part 12 moves toward the new fuel part 11 from the beginning to end of the burning cycle. That is, the core of the present embodiment performs CANDLE burning. The velocity of movement of the burning part 12 is roughly proportional to the power density and is inversely proportional to the fuel atomic number density.
The power density of the core in the present embodiment becomes higher at the center of the core. At the periphery of the core, leakage of neutrons becomes greater, so the power density becomes smaller the further toward the outside in the radial direction. For this reason, the position of the burning part in the axial direction is shifted more to the later position the further toward the outside in the radial direction.
The core 10 in the present embodiment includes the new fuel part 11, burning part 12, and burned up part 13. The new fuel part 11 is the part at which new fuel is arranged. The burning part 12 is a part at which neutrons are produced and the fuel burns. At the burning part 12, fission occurs whereby output is substantially produced. The burned up part 13 is a part which has burned up and almost no output is being produced.
At the core at the beginning of the n-th cycle, the new fuel part 11 is arranged at the bottom part of the core 10. The burning part 12 is arranged at the upper side of the new fuel part 11. At the burning part 12, fuel which already began burning at the previous cycle is arranged.
In the present embodiment, the burning part 12 arranged at the beginning of cycle becomes the part where burning is started. The fuel starts to burn from the burning part 12 and, as shown by the arrow 101, proceeds to burn in a direction toward the new fuel part 11. When the burning of n-th cycle proceeds and the end of cycle is reached, the burning part 12 proceeds down to the bottom end of the core 10. In the present embodiment, the burning is continued until almost all the new fuel part 11 is consumed. At the end of the burning cycle, the new fuel part 11 may remain.
In the present embodiment, depleted uranium is used as fuel. Depleted uranium contains about 99.8% of uranium 238 and about 0.2% of uranium 235. Uranium 238 absorbs neutrons and nuclear transformation occurs as shown in the following formula 1. Uranium 238 is transformed to plutonium 239.
In the vicinity of zero neutron fluence, uranium 238 absorbs neutrons whereby plutonium 239 is produced. Due to this, the infinite neutron multiplication factor rises. When reaching a predetermined neutron fluence, the ratio of the amount of plutonium 239 etc. to the amount of uranium 238 approaches a constant one, fission products (FP) build up, and the infinite neutron multiplication factor is gradually reduced. In this way, the fuel in the present embodiment has the property that the infinite neutron multiplication factor increases at the beginning of burning and the infinite neutron multiplication factor gradually decreases after that.
Further, the subcriticality of depleted uranium is large, so to make part of the core critical or more, a large amount of neutrons have to be made to be absorbed at the uranium 238. In the present embodiment, the core size is selected and the fuel assemblies and fuel rods are designed so as to satisfy these conditions.
By employing such a core configuration, it is possible to perform CANDLE burning. That is, it is possible to form a core wherein output is produced over the entire radial direction of the core and wherein a burning part is formed in part of the region in the axial direction of the core.
Referring to
When the n-th cycle ends, part of the burned up part of the fuel is taken out. At the core at the beginning of the (n+1)th cycle, as shown by the arrow 117, the burning part which is arranged at the bottom part of the core at the n-th cycle is arranged at the top part of the core and is used as the part for starting burning. At the core at the (n+1)th cycle, a new fuel part 11 is newly arranged at the bottom of the core. By replacing the fuel in this way, it is possible to burn fuel in the same way as the n-th cycle in the core at the (n+1)th cycle as well.
Next, the stopping of the nuclear reactor in the present embodiment will be explained. Referring to
By having the fuel assemblies 21b pulled out from the core 10, the leakage of neutrons from the core 10 becomes greater and the core 10 can be made subcritical and stopped. Referring to
Further, in the core 10 of the present embodiment, when stopping the nuclear reactor, the auxiliary members 51 are inserted into the core 10. By having the auxiliary members 51 inserted into the core, neutrons are absorbed at the auxiliary members 51. For this reason, the nuclear reactor can be made to stop more reliably.
The present embodiment is formed so that the movable fuel assemblies as a whole are pulled out from the core. Due to this configuration, the nuclear reactor can be made to stop more reliably. The amount of pullout of the movable fuel is not limited to this. If it is possible to stop the nuclear reactor by pulling out part of the movable fuel assemblies, the embodiment may also be formed so that part of the fuel assemblies is pulled out from the core.
Next, the startup of the nuclear reactor in the present embodiment will be explained. At the time of startup of the nuclear reactor, the movable fuel assemblies among the fuel assemblies are inserted into the core so as to achieve criticality and raise the power.
Referring to
When inserting the fuel assemblies 21b into the core 10, if moving the fuel assemblies 21b at a high speed, a large positive reactivity will be given to the core 10 and the power will suddenly rise in some cases. Therefore, when inserting the fuel assemblies 21b into the core 10, it is preferable to move the fuel assemblies 21b at a low speed. Alternatively, it is preferable to gradually insert the fuel assemblies 21b. For example, it is preferable to gradually insert the fuel assemblies 21b into the core 10 so that the power of the core rises by a predetermined rate.
At core of the nuclear reactor in the present embodiment, the nuclear reactor can be started and the nuclear reactor can be stopped even without using control rods. Channels for insertion of control rods to the core 10 become unnecessary and leakage of neutrons can be suppressed. For this reason, the criticality of the core can be easily achieved by CANDLE burning. Furthermore, the average power density of the core can be raised.
Further, if forming channels for insertion of control rods in the core 10, the integrated value of the power density in the axial direction of the core becomes smaller near the channels. Here, in the present embodiment, the integrated value of the power density in the axial direction of the core at any position in the radial direction is referred to as “axial direction integrated power”. Since the channels for insertion of control rods are not loaded with fuel, the axial direction integrated power ends up becoming smaller. For this reason, the burnup of the fuel which is arranged near the channels for insertion of control rods becomes smaller. The burning of fuel becomes uneven in the radial direction of the core.
In the core in the present embodiment, it is possible to eliminate the channels for insertion of control rods, so it is possible to make the axial direction integrated power approach a substantially constant state in the radial direction. That is, it is possible to make the power density distribution in the radial direction close to constant. Fuel can be made to burn more uniformly. Further, since the power density distribution in the radial direction can be made to approach a constant one, for example, operational control becomes easier and design of the nuclear reactor becomes easier.
The core of the present embodiment is formed so that movable fuel assemblies and auxiliary members are provided, the fuel assemblies are pulled out from the core, and auxiliary members are inserted into the core, but the invention is not limited to this. If possible to pull out and insert the movable fuel assemblies to stop and start the nuclear reactor, the auxiliary members need not be arranged. For example, by pulling out part of the fuel assemblies from the core, the leakage of neutrons from the core is made to increase and the amount of uranium which is arranged at the core can be reduced. For this reason, a large negative reactivity can be given to the core. Depending on the structure of the nuclear reactor, the nuclear reactor can be stopped and started even without arranging the auxiliary members.
Further, the auxiliary members in the present embodiment include an absorption substance which has the function of absorbing neutrons, but the invention is not limited to this. So long as being able to stop the nuclear reactor, the absorption substance need not be included. Even without the absorption substance being provided, the auxiliary members can be inserted into the core so as to maintain the mechanical strength of the core.
In the core, the movable fuel assemblies are arranged at the center region while the fuel assemblies which are fastened to the core are arranged in the peripheral region. Due to this configuration, the design of the movement apparatus for making the fuel assembly move can be simplified. Such a core is, for example, suitable for a small sized core with a small number of fuel assemblies.
The core in the present embodiment is formed so as to pull out the fuel assemblies in the center region from the core, but the invention is not limited to this. It may also be formed so as to pull out the fuel assemblies which are arranged at the peripheral region from the core. The number of fuel assemblies which are pulled out can be determined so as to enable the nuclear reactor to be started up and stopped. Further, the arrangement of the movable fuel assembly is not limited to the above embodiment. They may be arranged at any positions.
The core in the present embodiment is configured so as to pull out the movable fuel assemblies toward the bottom side, but the invention is not limited to this. The movable fuel assemblies may also be formed so as to be pulled out toward the top side of the core.
Further, the fuel assemblies in the present embodiment are formed to regular hexagonal prism shapes, but the invention is not limited to this. Any shapes of fuel assemblies may be employed. For example, to facilitate pullout and insertion of the fuel assemblies, the fuel assemblies may be tapered so as to gradually change in length along the longitudinal direction.
The auxiliary members in the present embodiment have structures similar to the fuel assemblies except for the substance which is arranged inside of the cladding materials, but the invention is not limited to this. As the auxiliary members, ones of any structures may be employed. The insides of the cladding materials may also be empty.
The fuel in the present embodiment was explained with reference to depleted uranium as the new fuel which was loaded into the core, but the invention is not limited to this. It is also possible to use at least one of natural uranium and depleted uranium to perform CANDLE burning. Further, the present invention can also be applied to any fast neutron reactor which enables CANDLE burning.
In the present embodiment, the burning part of the previous cycle was arranged at the top of the new fuel part at the beginning of the burning cycle, but the invention is not limited to this. The new fuel part can be arranged at either end of the burning part in the axial direction of the core. Furthermore, new fuel parts may be arranged at the two ends of the burning part.
Further, in the present embodiment, the part starting to burn at the beginning of a cycle uses the fuel which was arranged at the bottom of the core at the end of the cycle of the previous cycle, but the invention is not limited to this. The part starting to burn at the beginning of a cycle may also be formed so as to produce neutrons. For example, fuel containing a predetermined concentration of plutonium or enriched uranium etc. may also be arranged. Further, neutrons may be supplied from the outside to cause burning to start.
Further, in the core in the present embodiment, the axial direction of the core is parallel with the vertical direction, but the invention is not limited to this. The axial direction of the core may also be parallel to the horizontal direction. That is, it is also possible to lay the core in the present embodiment sideways.
In the present embodiment, the explanation was given with reference to the example of a method of operation not controlling the reactivity of the core when the fuel is burning steadily, but the invention is not limited to this. It is also possible to control the reactivity.
In the present embodiment, the explanation was given with reference to the example of a core of a nuclear reactor used in a electric power generation facility, but the invention is not limited to this. It is possible to apply the present invention to a nuclear reactor in any facility. For example, it is possible to use the core of the nuclear reactor of the present invention as the power source for a ship etc.
In the above figures, the same or corresponding parts are assigned the same reference numerals. Note that, the above embodiments are illustrations and do not limit the invention. Further, in the embodiments, changes included in the claims are intended.
Number | Date | Country | Kind |
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2011-001865 | Jan 2011 | JP | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/JP2012/050112 | 1/5/2012 | WO | 00 | 7/17/2013 |