1. Field of the Invention
The present invention relates to a nuclear power plant, a fuel pool water cooling facility and a fuel pool water cooling method.
2. Description of the Related Art
A boiling water reactor stores not only reactor fuel being used in a reactor pressure vessel but also spent fuel having been operated for several cycles. A reactor building for a boiling water reactor is hereinafter abbreviated as BWR. Spent fuel is generally stored in the fuel pool water (cooling water) in a fuel pool (hereinafter abbreviated as SFP) provided in a reactor building (see JP-9-329684-A). In general, this type of BWR has a circulating water system for maintaining fuel pool water at an appropriate temperature. The fuel pool water is forcibly circulated by a pump between a cooling water tank and the like and a fuel pool or by other means in order to remove the residual heat of fuel. For example, the fuel pool water is cooled through heat exchange with sea water in the process of the circulation. In this way, the water temperature in the fuel pool is maintained at approximately 40° C.
From the standpoint of enhancing the safety of the BWR, it is essential to surely implement three principles (1. stop of fission, 2. cooling of reactor fuel, 3. confinement of radioactive materials) for ensuring the safety of a reactor in case of emergency. For item 2. cooling of reactor fuel, a multiple safety protection system is specially installed to take effective actions against emergencies. The multiple safety protection system includes an emergency core cooling system (ECCS), a residual heat removal system (RHR), an isolation condenser (IC) and a passive containment cooling system (PCCS).
However, if station black out occurs due to unpredictable circumstances and a circulating water system is shut down, a problem with cooling of the fuel pool water will arise. Specifically, if, during the time elapsing until emergency power will be recovered, water temperature increases to atmospheric saturation temperature (approximately 100° C.), then the water in the fuel pool will evaporate and the water level of the fuel pool will lower.
The present invention has been made in view of such situations and aims to provide a nuclear power plant and a fuel pool water cooling facility and method that can suppress the decreasing of the water level in a fuel pool with no power supply at the time of malfunction of a circulating water system.
To solve the above problem, the present invention is configured such that a heat pipe transfers the heat of a fuel pool and discharges it to the atmosphere.
According to the present invention, even in the event that the circulating water system adapted dynamically to cool fuel pool water malfunctions, the heat pipe transfers the heat of the fuel pool water and discharges it to the atmosphere. In this way, the boiling and evaporation of the fuel pool water can be suppressed to suppress the decreasing of the water level of the fuel pool.
Preferred embodiments of the present invention will hereinafter be described with reference to the drawings.
A reactor building 10 in the BWR power plant shown in
The pressure suppression pool 4 of a donut type is connected to the lower portion of the containment vessel 3. A conduit pipe is connected to the upper portion of the reactor pressure vessel 2 and extends into liquid 4a in the pressure suppression pool 4. For example, if the pressure in the reactor pressure vessel 2 is raised, steam can be discharged into the liquid 4a in the pressure suppression pool 4 for condensation by opening a main steam relief safety valve attached to the conduit pipe. If the pressure in the containment vessel 3 is further raised, the steam in the containment vessel 3 is discharged through a vent pipe 7 of containment vessel (drywell) or a vent pipe 8 of containment vessel (wetwell). The steam thus discharged is passed through a radioactive material adsorption filter 60 and radioactive materials are recovered. Then, the steam is discharged from an exhaust tower 9 to the outside of the plant, i.e., to the atmosphere. The above-mentioned isolation condenser 5 is installed at a height approximately equal to the upper portion of the containment vessel 3 in the reactor building 10.
The above-mentioned SFP 11 is installed at a height approximately equal to the upper portion of the containment vessel 3 in the reactor building 10. The spent fuel 12 is installed in a lower portion of the SFP 11. Fuel pool water 14 is stored in the SFP 11 at a level twice or more the height (e.g. approximately 4 m) of the bundle of the spent fuel 12. The BWR power plant is provided with a circulating water system 21 for dynamically cooling the fuel pool water 14 of the SFP 11. The SFP 11 is connected to a water source (not shown) such as a tank and the like installed through a feed water root 21a and drainage 21b. The fuel pool water 14 is forcibly circulated by driving a pump 22 between the SFP 11 and the water source through the feed water root 21a and the drainage 21b. In other words, the fuel pool water 14 having taken the residual heat of the spent fuel 12 in the SFP 11 is discharged from the SFP 11 through the drainage 21b. In addition, the fuel pool water 14 from the water source via the feed water root 21a flows into the SFP 11. In this way, the fuel pool water 14 in the SFP 11 is maintained at a predetermined temperature (e.g. approximately 40° C.). The fuel pool water 14 circulated between the SFP 11 and the water source is subjected to heat exchange with seawater 24a pumped up from the sea by a pump 25 by use of a cooling water heat exchanger 23 installed in the middle of the circulating system (the drainage 21b in the present embodiment). Thus, the heat of the fuel pool water 14 is transferred to seawater. The seawater 24b having taken heat in the cooling water heat exchanger 23 is discharged to the sea. In short, seawater serves as a final heat sink for the residual heat of the spent fuel 12.
Incidentally, the SFP 11 not only stores the spent fuel 12 but also temporarily stores the fuel in use taken out of the reactor pressure vessel 2 for a periodic inspection in some cases.
At least one heat pipe 13 is installed in the SFP 11 so as to have one side (on the lower side in the present embodiment) submerged in the fuel pool water 14 stored therein. The heat pipe 13 is designed as below. The evaporation and condensation of working fluid occurs in the inner space of the heat pipe 13. Latent heat resulting from such evaporation and condensation are used to transfer the residual heat transferred to the fuel pool water 14 from the spent fuel 12, to the outside of the SFP 11 through the heat pipe 13. The heat pipe 13 has the other side (the upper side in the present embodiment) exposed to the inside of the passage of an air duct 42 installed on the reactor building 10. The installation location of the heat pipe 13 with respect to the reactor building 10 is not always restrictive. However, the present embodiment exemplifies the case where the heat pipe 13 is installed on a lateral external wall portion 10a of the reactor building 10. The air duct 42 is such that one of openings is located at a position higher than the other. The present embodiment exemplifies the vertically extending straight pipe. In this case, in the air duct 42, air heated with heat inputted from the heat pipe 13 moves upward. Therefore, because of natural circulation, air 18a outside the reactor building 10 enters at the inlet (the lower opening) of the air duct 42 and heated air 18b flows out of the outlet (the upper opening) of the air duct 42. In this way, residual heat is finally discharged to the atmosphere.
The heat pipe 13 shown in
In the heat pipe 13 in
The heat pipe 13 shown in
Also in the heat pipe 13 in
The forced circulation of the fuel pool water 14 by the pump 22 may be shut down due to station black out. In such an event, if the water temperature in the SFP 11 rises up to approximately 60° C., it is necessary to rapidly improve the residual heat removal performance of the heat pipe 13 so as to prevent the boiling of the fuel pool water 14 in the SFP 11. To meet the necessity, water is selected as working fluid in the heat pipe 13 and saturated pressure P in the heat pipe 13 is made to satisfy the following condition:
P≦20 kPa (Expression 1)
If the saturated pressure P in the heat pipe 13 is 20 kPa, the working fluid boils at approximately 60° C. The reason for using water as working fluid is that water has large latent heat and the same components as those of the fuel pool water 14. Thus, there is an advantage that problem with fluid-mixing doesn't arise, even if the heat pipe 13 should be damaged.
The spent fuel 12 releases residual heat of about several percentage of the thermal power in operation. The fuel pool water 14 in the SFP 11 is heated with the residual heat. The heat pipe 13 is heated with the fuel pool water 14 in the heating part 31 to raise the water temperature of the liquid 36 to approximately 60° C. At this time, the steam flow 37 is generated from the liquid 36, heat transfer is started. In the reactor building 10, the steam flow 37 has no heat loss in an adiabatic part 32 of the heat pipe 13 that is exposed from the surface of the fuel pool water 14 while keeping rising in the heat pipe 13. When rising up to the cooling part 33 being exposed to the outside of the reactor building 10, the steam flow 37 is subjected to heat exchange with the air 18b to be cooled to e.g. approximately 25° C. If the so-called cooling-reinforcing temperature Tc is 60° C., the liquid 36 functions as a thermal diode in which the heat transfer performance of the heat pipe 13 is exhibited, only after the liquid 36 reaches the cooling-reinforcing temperature Tc. Incidentally, there is no problem in setting, at an appropriate value lower than 60° C., the above-mentioned cooling-reinforcing temperature Tc at which the heat pipe 13 produces a cooling switching effect.
In
On the other hand, in the present embodiment (a solid line), even if the forced circulation cooling function of the pump 22 lowers, the temperature of the fuel pool water 14 rises to the cooling-reinforcing temperature Tc (=approximately 60° C.) at which the evaporation and condensation phenomenon of the working fluid (water) occurs in the heat pipe 13 at time t=t1 (<t2). Then, the cooling function of the heat pipe 13 starts to act quickly and thereafter the surface temperature of the fuel pool water 14 is maintained at approximately Tc. At this time, the fuel pool water 14 in the SFP 11 causes natural convection. Therefore, the evaporation of the fuel pool water 14 in the SFP 11 is suppressed to maintain the fuel pool water 14 at the level of the initial time (time t=t0). Thus, the sufficient water level of the SFP 11 is ensured and also the temperature of the fuel pool water 14 can be maintained at approximately Tc (=approximately 60° C.).
In the nuclear power plant of the present embodiment as described above, the residual heat of the spent fuel is cooled by the heat exchange of the fuel pool water 14 of the SFP 11 with the cooling water forcibly circulated through the circulating water system 21. In addition, the residual heat of the spent fuel is cooled by the heat transfer by means of the heat pipe 13 installed in the SFP 11. The heat transfer by the heat pipe 13 needs no power. Phase-change phenomena of working fluid such as boiling and condensation are employed. Therefore, the heat transfer performance of the working fluid having large latent heat is remarkably higher than that of another cooling means in which working fluid is naturally circulated as a liquid single-phase flow. Even if the pump 22 has a malfunction due to station black out, the heat pipe 13 can statically release the heat of the fuel pool water 14 through natural circulation. The fuel pool water 14 is prevented from being evaporated so that the water level of the SFP 11 does not lower and the spent fuel 12 is not exposed from the water surface. Thus, the heat removal of the spent fuel 12 can be continued to thereby achieve the safety and reliability of the spent fuel 12 stored in the fuel pool water 14.
The second embodiment is different from the first embodiment in the following point. The heating part 31 of the heat pipe 13 in the first embodiment does not reach the spent fuel rod 12 in the fuel pool water 14. On the other hand, a heat pipe 13A in the present embodiment is inserted between a plurality of spent fuel rods 12 in the fuel pool water 14.
More specifically, as shown in
In the present embodiment, the insert part 31a is inserted between the spent fuel rods 12 installed in the SFP 11 in such a manner that the heat-absorbing plates 31aa cover the overall height-range of the spent fuel rods 12.
The other configurations are the same as those of the first embodiment. The same portions are denoted by like reference numerals in the above-mentioned figures and their explanations are omitted.
The tendency of temperature gradients is the same as that of the first embodiment. However, as seen from the comparison with
The third embodiment is different from the first embodiment in the following point. A pool 15 for storage of reactor core internal structure is installed in a reactor building 10. The pool 15 is used to store a reactor core internal structure in pool water 15a. In addition, a heat pipe 17 for the pool for storage of reactor core internal structure is additionally mounted to the pool 15. The pool 15 is connected to the SFP 11 by way of a connecting heat pipe 16.
The pool 15 is installed at a height equal to the upper portion of the containment vessel 3 in the reactor building 10. The basic configurations of the heat pipe 17 for storage of reactor core internal structure and of the connecting heat pipe 16 are the same as that of the heat pipe 13 for the fuel pool.
The other configurations are the same as those of the first embodiment. The same portions are denoted by like reference numerals in the above-mentioned figures and their explanations are omitted.
In the present embodiment, the residual heat of the spent fuel 12 is released by the heat removal through the circulating water system 21 and the heat removal through the heat pipe 13 for the SFP 11. In addition, the residual heat of the spent fuel 12 is released by heat removal through a heat transfer route from the connecting heat pipe 16 via the pool 15 for storage of reactor core internal structure to the heat pipe 17. Thus, the present embodiment can improve a passive cooling capacity even compared with the first embodiment.
The fourth embodiment is different from the first embodiment in the provision of a blast fan 41 adapted to deliver air to the cooling part of the heat pipe 13. In other words, this is an example in which the cooling part 33 of the heat pipe 13 is changed from a natural cooling method to a forced air cooling method using the blast fan 41. In the present embodiment, the blast fan 41 is installed inside the air duct 42 so as to locate on the upstream side (on the lower side) of the air flow direction in the air duct 42 with respect to the cooling part 33 of the heat pipe 13. However, the blast fan 41 may locate on the downstream side. The blast direction is an upward direction.
The other configurations are the same as those of the first embodiment. The same portions are denoted by like reference numerals in the above-mentioned figures and their explanations are omitted.
The cooling part 33 of the heat pipe 13 is provided with a large number of the cooling fins (the cooling means 34, see
Also in the present embodiment, the residual heat of the spent fuel 12 can be released by the heat removal of two types: the heat removal through the circulating water system 21 and the heat removal through the heat pipe 13. If the blast fan 41 is driven, the cooling efficiency of the heat pipe 13 is improved, thereby producing a higher cooling effect.
The fifth embodiment is different from the first embodiment in that the heat pipe 13 is not normally submerged in the fuel pool water 14 but is submerged as needed.
In the present embodiment, the heat pipe 13 is provided with retaining portions 61 and 62 on the lower side of the cooling part 33 and at a lower end of the heat pipe 13, respectively. A plurality of heat pipes 13 are bundled and unitized by the retaining portions 61, 62 and the cooling means 34. However, the plurality of heat pipes 13 are not always required. The present embodiment has a stopper 45 which supports the heat pipes 13 at a position above the water surface of the SFP 11 and which can input the heat pipes 13 in the fuel pool water 14 of the SFP 11 by releasing the support of the heat pipes 13. The stopper 45 is installed in the upper portion of the reactor building 10 so as to support the upper side retaining portion 61 during normal times. In this state, the heat pipes 13 are wholly located above the surface of the fuel pool water 14, i.e., are not submerged in the fuel pool water 14.
However, when the stopper 45 is removed to release the support of the retaining portion 61 by the stopper 45, the heat pipes 13 are driven to a position at which the lower side retaining portion 62 is supported by the stopper 46 installed on the inner wall of the SFP 11 (the state in
Although particularly not shown, the heat pipe 13 may be configured to pass through a ceiling part of the reactor building 10 in a lower portion below the stopper 45. In such a case, the cooling part 33 may be configured to be exposed to the outside of the reactor building 10 even in the state in
The other configurations are the same as those of the first embodiment. The same portions are denoted by like reference numerals in the above-mentioned figures and their explanations are omitted.
In the present embodiment, in case of a loss of power for the circulating water system 21, the stopper 45 is removed to allow the heat pipes 13 to be gravity-driven. This makes it possible for the heat pipes 13 to cool the fuel pool water 14. Thus, the present embodiment can produce the same effect as that of the first embodiment.
The sixth embodiment is different from the first embodiment in that the fuel pool water 14 in the SFP 11 is sealed. More specifically, an upper plate 51 is installed on the SFP 11 to seal the fuel pool water 14 in the SFP 11. Thus, generated steam containing radioactive materials resulting from residual heat removal is confined in the SFP 11. The heat pipe 13 passes through the upper plate 51.
The other configurations are the same as those of the first embodiment. The same portions are denoted by like reference numerals in the above-mentioned figures and their explanations are omitted.
Measures are taken to prevent the boiling of the fuel pool water 14 by means of the heat pipe 13. However, in the event that the fuel pool water 14 is boiled and evaporated by the residual heat of the spent fuel 12, if the SFP 11 is opened, steam flows out of the SFP 11 so that the water level of the SFP 11 probably lowers. On the other hand, the upper plate 51 is installed on the SFP 11; therefore, the steam of the fuel pool water 14 is prevented from escaping to the outside of the SFP 11 so that the water level of the SFP 11 may not lower.
The seventh embodiment is different from the sixth embodiment in the following point. Hydrogen concentration in a gaseous phase in the SFP 11 is detected. Hydrogen gas is released to the atmosphere in the range where the hydrogen concentration thus detected does not exceed a flammability limit of hydrogen concentration.
A nuclear power plant of the present embodiment includes a hydrogen concentration detector 52, a hydrogen emission conduit 55 and a control valve 54. The hydrogen concentration detector 52 detects the hydrogen concentration in gaseous phase space in the SFP 11. The hydrogen emission conduit 55 connects the gaseous space in the SFP 11 with the external space of the reactor building 10. The control valve 54 opens and closes the passage of the hydrogen emission conduit 55. The SFP 11 is provided with a mouth detection 53 connecting with the gaseous phase space of the SFP 11. This mouth detection 53 is connected to the hydrogen concentration detector 52. Although particularly not shown, it may be determined that the discharge of hydrogen 56 is necessary on the basis of the hydrogen concentration detected by the hydrogen concentration detector 52. In such a case, only if the hydrogen concentration is at a level equal to or above the flammability limit of hydrogen concentration for reaction with oxygen in air, a control signal is sent to the control valve 54. Then, the control valve 54 opens the hydrogen emission conduit 55, thereby discharging hydrogen 56 via the hydrogen emission conduit 55. Although particularly not shown, it is conceivable that a control facility is installed which controllably opens and closes the control valve 54 on the basis of a detection signal of the hydrogen concentration detector 52.
The other configurations are the same as those of the sixth embodiment. The same portions are denoted by like reference numerals in the above-mentioned figures and their explanations are omitted.
The present embodiment can produce the same effect as that of the sixth embodiment and can suppress the generation of hydrogen combustion in the SFP 11.
The description has been given thus far taking, as an example, the case where the present invention is applied to the BWR. However, the present invention can be applied not only to the BWR but to plants that have a fuel pool. The present invention may be applied to another type of a nuclear power plant such as a pressurized water reactor or a fast breeder reactor. Also such a case can produce the same effect as the case where the present invention is applied to the BWR.
The embodiments can arbitrarily be combined with each other and can be modified in design in a range not departing from the technical concept of the present invention.
Number | Date | Country | Kind |
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2011-100002 | Apr 2011 | JP | national |