METHOD FOR IMPROVING THE WITHSTANDING CAPABILITY OF THE CLADDING MATERIAL IN THE FAST NEUTRON IRRADIATION ENVIRONMENT
20230335304 · 2023-10-19
Inventors
- Di Yun (Xi' an, CN)
- Zhaohao Wang (Xi' an, CN)
- Chunyang Wen (Xi' an, CN)
- Tiantian Shi (Xi' an, CN)
- Linna Feng (Xi' an, CN)
- Wenbo Liu (Xi' an, CN)
- Jianqiang Shan (Xi' an, CN)
Cpc classification
G21C21/02
PHYSICS
G21C1/02
PHYSICS
International classification
G21C3/18
PHYSICS
G21C1/02
PHYSICS
Abstract
The invention belongs to the technical field of nuclear reactor materials design, and discloses a method for improving the withstanding capability of the cladding material in the fast neutron irradiation environment, comprising the following steps: selecting the cladding material with the annular structure and placing it on the outer side of the metallic fuel slug, with leaving a 0.2-0.8 mm gap between the metallic fuel slug and the cladding material; processing the operation in a reactor subsequently, with an annealing process of the fast neutron reactor fuel during the operation of the reactor; improves the withstanding capability of the cladding material in the fast neutron irradiation environment. The invention processes annealing treatment of the cladding material by balancing the internal and external stresses, multiple cycles of steady-state and transient operations, enhancing the withstanding capability of the steel in the high neutron irradiation environment, improving the lifetime of the cladding material.
Claims
1. A method for improving the withstanding capability of the cladding material in the fast neutron irradiation environment, wherein comprises the following steps: selecting the cladding material with the annular structure and placing it on the outer side of the metallic fuel slug, with leaving a 0.2-0.8 mm gap between the metallic fuel slug and the cladding material; processing the operation of fast neutron reactor fuel material in a reactor subsequently, with an annealing process of the fast neutron reactor fuel during the operation of the reactor; and during the annealing process, the gas pressure of both inner surface and the outer surface of the cladding material are adjusted separately to obtain the force equilibrium, which improves the withstanding capability of the cladding material in the fast neutron irradiation environment; the cladding material is steel material.
2. The method of claim 1, wherein the regulation of the inner surface gas pressure, and the outer surface gas pressure as well, of the cladding material is achieved by the following steps: applying the external pressure to the cladding material by means of the primary circuit in the reactor core; providing a gas channel at the top of the gas plenum of the clad material connected to the gas plenum of the clad material, and providing a pressure plug in the gas channel; the pressure plug is provided in the shape of an umbrella cover and the inner wall of the pressure plug is in contact with the liquid metal coolant of the primary circuit; the gas pressure discharging the liquid metal from the pressure plug thereby released to the primary circuit, when the pressure in the gas chamber of the cladding material is 4.3 to 10.3 MPa; and the pressure becomes less once the gas is released, therefore the liquid metal of the primary circuit re-enters the inner wall side of the pressure plug lid to seal the remaining gas, to guarantee the precise control of the gas pressure in the gas plenum by setting the mass of the pressure plug.
3. The method of claim 2, wherein the pressure in the primary circuit is 3 to 8 MPa.
4. The method of claim 1, wherein the metallic fuel slug adopts the high burnup U-50Zr metal fuel with periodic fission gas release.
5. The method of claim 1, wherein the annealing process is carried out by a plurality of cycles, and one cycle is a steady-state operation followed by a transient operation.
6. The method of claim 5, wherein the steady-state operation is converted to a transient operation when the irradiation damage to the cladding material is in the swelling incubation period and before significant embrittlement occurs.
7. The method of claim 5, wherein the temperature of the steady-state operation is at 400 to 600° C.
8. The method of claim 5, wherein the temperature of the transient operation is at 700 to 850° C.
9. The method of claim 5, wherein the period of the transient operation is 6 to 8 hours.
10. The method of claim 5, wherein before performing the first low temperature steady state operation, prefilling the gas plenum of the cladding material until the internal pressure of the gas plenum is 1 MPa.
Description
4. BRIEF DESCRIPTION OF ACCOMPANY DRAWINGS
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5. SPECIFIC EMBODIMENT OF THE INVENTION
[0043] To make the technical solutions provided by the invention more comprehensible, a further description of the invention is given below in combination with the attached drawings and embodiments, and the embodiments are exemplary and not the limitations of the scope of the disclosure.
Embodiment 1
[0044] The embodiment provides a method for improving the withstanding capability of the cladding material in the fast neutron irradiation environment, comprising the following steps: [0045] selecting the metallic fuel slug with an annular geometry, an inner central hole diameter of 1 mm, and a fuel slug outer diameter of 9 mm as the fuel of the embodiment. [0046] selecting the cladding material with an annular geometry, an inner diameter of 8 mm and an outer diameter of 11 mm; providing a gas channel at the top of the gas chamber of the clad material connected to the gas plenum of the clad material, and providing a pressure plug in the gas channel, to obtain the cladding material of the embodiment.
[0047] The embodiment comprises the following steps: applying the external pressure to the cladding material by means of the primary circuit in the reactor core; the pressure plug is provided in the shape of an umbrella cover and the inner wall of the pressure plug is in contact with the liquid metal coolant of the primary circuit; directly calculating the upper pressure limit according to the gas pressure, steady-state operation and annealing temperature of primary circuit after using the relationship PV=nRT; when the pressure in the gas chamber reaches this pressure limit, such as 7.3 MPa, the gas pressure discharges the liquid metal from the pressure plug thereby released to the primary circuit; and the pressure becomes less until the gas plenum pressure returns to the set upper limit once the gas is released, therefore the liquid metal of the primary circuit re-enters the inner wall side of the pressure plug lid to seal the remaining gas, to guarantee the precise control of the gas pressure in the gas plenum by setting the mass of the pressure plug; the pressure plug mass m is determined by the pressure value of the pressure set in primary circuit and the high temperature pressure balance, that is m×g/S=P.sub.in.
[0048] Wherein S is the surface stressed area under the pressure plug, and [0049] the P.sub.in is the set internal pressure of fuel rod, determined by the primary circuit pressure: P.sub.in=P.sub.out, and [0050] the P.sub.out is the temperature in the annealed condition of the primary circuit, determined by the steady-state operating pressure of the primary circuit P.sub.1: P.sub.out/T.sub.t=P.sub.1/T.sub.s, and [0051] T.sub.s is the outlet temperature for the steady-state operation of the primary circuit, and [0052] T.sub.t is the temperature of the primary circuit annealing operation, and [0053] P.sub.1 is the pressure of the primary circuit steady-state operation.
[0054] Providing the cladding material on the outer side of the fuel slug, with leaving a 0.5 mm gap between the fuel and the cladding material and to obtain the fast neutron reactor fuel material of the embodiment.
[0055] When the first steady-state operation of the fast neutron reactor fuel material of the embodiment in the reactor, the fuel slug and the cladding will not come into contact and the fission gas has not been released because the fuel slug is in a low-temperature low swelling state; therefore, there is no fission gas pressure in the cladding, and the fuel is prefilled with 1 MPa of gas to keep it in basic balance with the external pressure; a slightly higher external pressure slowly creep the cladding inward. The reactor core operation state of the steady-state operation is artificially adjusted when the irradiation damage to the cladding material is in the swelling incubation period and before occurring the significant embrittlement, to achieve the primary circuit coolant temperature rise from 500° C. in steady-state operation to 880° C. in transient operation (reactor 0 power operation). The warming process is accompanied by a greater thermal expansion of the cladding than the fuel expansion, widening the fuel-cladding gap and rising the fuel temperature to 900° C. At the same time, the increase in coolant temperature increases the fuel temperature to drive a large fractional release of fission gas, causing the pressure inside the cladding to increase to the maximum internal pressure controlled by the pressure plug. The maximum pressure set by the pressure plug at the top of the cladding is equal to the pressure in the primary circuit at the maximum planned operating temperature of the cladding at transient operation. In this way, the internal and external pressures achieve complete equilibrium when the cladding temperature rises to the specified annealing temperature (at this time the reactor is in 0 power operation and the only heat generated inside the fuel is the residual decay heat, thus, the coolant axial temperature difference is only 10-20° C.). Due to the massive release of fission gas, the fuel swelling is not obvious, and the fuel-cladding gap is still open. The cladding is annealed for 7 hours in this high-temperature transient operating condition to restore plasticity and recover the irradiation defects. At the end of the high temperature transient operation, the thermodynamic hydraulic operation state is artificially adjusted to cool down the coolant and the reactor is restarted and reaches its rated power. During the cooling process, the fuel shrinkage is smaller than cladding shrinkage, but the fuel and cladding are still not in contact due to the initially set fuel-cladding gap. As the coolant temperature decreases causing the external pressure to drop, and thus the internal gas pressure is slightly greater than the external gas pressure, the cladding creeps outward in small increments until the temperature returns to steady-state operation. The fuel returns to a low swelling spinodal decomposition two-phase state for the second steady-state operation. As shown in
Embodiment 2
[0056] The embodiment provides method for improving the withstanding capability of the cladding material in the fast neutron irradiation environment and the differences between the embodiment and Embodiment 1 are as follows:
[0057] In the embodiment, selecting the fuel slug with an annular geometry, an inner central hole diameter of 0.2 mm, and a fuel slug outer diameter of 5 mm.
[0058] In the embodiment, selecting the cladding material with an annular geometry, an inner central hole diameter of 5.2 mm, and a fuel slug outer diameter of 6.2 mm.
[0059] In the embodiment, leaving 0.2 mm between the fuel and the cladding material.
[0060] In the embodiment, the steady-state operation temperature for each per cycle is 400° C.
[0061] In the embodiment, the transient operation temperature for each cycle is 700° C. and the transient operation period is 6 hours.
[0062] In the embodiment, the fuel-cladding gap opens again during the 7th transient operation ramp-up and high-temperature constant temperature operation, therefore the cladding is still relatively safe for the transient operation. However, when entering the steady-state operation phase in the 8th operating cycle, there may be a risk of cladding failure and reactor shutdown due to continuous creep of the fuel-cladding contact outward.
Embodiment 3
[0063] The embodiment provides method for improving the withstanding capability of the cladding material in the fast neutron irradiation environment and the differences between the embodiment and Embodiment 1 are as follows:
[0064] In the embodiment, selecting the fuel slug with an annular geometry, an inner central hole diameter of 2 mm, and a fuel slug outer diameter of 13 mm.
[0065] In the embodiment, selecting the cladding material with an annular geometry, an inner central hole diameter of 13.8 mm, and a fuel slug outer diameter of 15.8 mm.
[0066] In the embodiment, leaving 0.8 mm between the fuel and the cladding material.
[0067] In the embodiment, the steady-state operation temperature for each per cycle is 600° C.
[0068] In the embodiment, the transient operation temperature for each cycle is 850° C. and the transient operation period is 8 hours.
[0069] In the embodiment, the 10th low-temperature operation after 9 cycles of operation results in contact between the fuel and the cladding due to the continuous swelling of the fuel slug, which causes the cladding to start creeping outward slowly (low temperature and low creep). the fuel-cladding gap opens again during the 9th transient operation ramp-up and high-temperature constant temperature operation, therefore the cladding is still relatively safe for the transient operation. However, when entering the steady-state operation phase in the 10th operating cycle, there may be a risk of cladding failure and reactor shutdown due to continuous creep of the fuel-cladding contact outward.
[0070] The above embodiments are only to illustrate the technical idea of the invention and not intended to limit the scope of protection of the invention. Any transformations made on the basis of technical solutions with the technical ideas of the invention will fall within the scope of protection of the invention; the technology not covered by the invention can be realized by the prior art.
[0071] The above description of the invention and the embodiments thereof is not restricted, and the accompanying drawings are only one of the embodiments of the invention, and the actual structure is not limited thereto. In conclusion, the similar structures and embodiments with the technical scheme of the invention, which are designed by the general skilled person in the art inspired by the invention, without creativity and without departing from the spirit of the invention, should be included in the protection scope of the invention.