Abstract
Space nuclear reactor power (SNRP) using a gas-cooled reactor (GCR) and a closed Brayton cycle (CBC) is the ideal choice for future high-power space missions. To investigate the safety characteristics and develop the control strategies for gas-cooled SNRP, transient models for GCR, energy conversion unit, pipes, heat exchangers, pump and heat pipe radiator are established and a system analysis code is developed in this paper. Then, analyses of several operation conditions are performed using this code. In full-power steady-state operation, the core hot spot of 1293 K occurs near the upper part of the core. If 0.4 $ reactivity is introduced into the core, the maximum temperature that the fuel can reach is 2059 K, which is 914 K lower than the fuel melting point. The system finally has the ability to achieve a new steady-state with a higher reactor power. When the GCR is shut down in an emergency, the residual heat of the reactor can be removed through the conduction of the core and radiation heat transfer. The results indicate that the designed GCR is inherently safe owing to its negative reactivity feedback and passive decay heat removal. This paper may provide valuable references for safety design and analysis of the gas-cooled SNRP coupled with CBC.
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Abbreviations
- A :
-
Flow area/m2
- C :
-
Delayed neutron precursor concentration/m−3
- c p :
-
Specific heat capacity/(J · kg−1·K−1)
- D :
-
Hydraulic diameter/m
- E :
-
Effective energy fraction
- f :
-
Friction coefficient
- H :
-
Height/m
- h :
-
Heat transfer coefficient/(W·m−2·K−1)
- I :
-
Moment of inertia/(kg·m2)
- k :
-
Thermal conductivity (W · m−1 · K−1)
- m :
-
Mass/kg
- M:
-
Number
- N :
-
Shaft speed (rad · s−1)
- Nu :
-
Nusselt number
- P :
-
Power/W
- Pr :
-
Prandtl number
- p :
-
Pressure/Pa
- Q :
-
Volumetric heat generation/(W · m−3)
- R :
-
Radius/m
- R g :
-
Gas constant/(J · kg−1 · K−1)
- Re :
-
Reynolds number
- r :
-
Radial coordinate/m
- S :
-
Area/m2
- T :
-
Temperature/K
- t :
-
Time/s
- V :
-
Volume/m3
- W :
-
Mass flow rate/(kg · s−1)
- z :
-
Axial coordinate/m
- ρ :
-
Reactivity (Δk·k−1); Density/(kg · m−3)
- λ :
-
Decay constant/s−1
- Λ :
-
Neutron generation time/s
- β :
-
Delayed neutron fraction
- ε :
-
Emissivity
- α :
-
Reactivity feedback coefficient/(Δk·k−1 · K−1)
- σ :
-
Stefan-Boltzmann constant/(5.67 × 10−8 W·m−2·K−4)
- alt:
-
Alternator
- b:
-
Core block
- bin:
-
Core block inner surface
- bout:
-
Core block outer surface
- bv:
-
Core block and pressure vessel
- com:
-
Compressor
- Cin:
-
Compressor inlet
- Cout:
-
Compressor outlet
- d:
-
Downcomer
- db:
-
Downcomer and core block
- decay:
-
Decay
- din:
-
Downcomer inner
- dout:
-
Downcomer outer
- dv:
-
Downcomer and pressure vessel
- eff:
-
Effective
- f:
-
Fuel pin
- fb:
-
Fuel pin and core block
- fiss:
-
Fission
- fout:
-
Fuel pin outer surface
- g:
-
He-Xe gas
- gb:
-
Gas and core block
- gf:
-
Gas and fuel pin
- i :
-
delayed neutron group
- iavg:
-
Average
- in:
-
External reactivity
- inner:
-
Inner surface
- iref:
-
Reference
- j :
-
Fission product group
- n:
-
Component
- outer:
-
Outer surface
- p:
-
Annular gas passage
- pin:
-
Gas passage inner
- pout:
-
Gas passage outer
- pv:
-
Pressure vessel
- pvin:
-
Pressure vessel inner surface
- pw:
-
Plate wall
- pwH:
-
Plate wall high-pressure side
- pwL:
-
Plate wall low-pressure side
- r:
-
Radial reflector
- rout:
-
Radial reflector outer surface
- RCH:
-
Recuperator high-pressure side
- RCL:
-
Recuperator low-pressure side
- RCP:
-
Recuperator passage
- s:
-
Solid
- shaft:
-
TAC shaft
- sp:
-
Space environment
- Tin:
-
Turbine inlet
- Tout:
-
Turbine outlet
- tur:
-
Turbine
- x:
-
Core block ring
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Acknowledgements
This work was supported by the National Natural Science Foundation of China (Grant No. U1967203), the National Key R&D Program of China (Grant No. 2019YFB1901100) and China Postdoctoral Science Foundation (Grant No. 2019M3737).
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Wang, C., Zhang, R., Guo, K. et al. Dynamic simulation of a space gas-cooled reactor power system with a closed Brayton cycle. Front. Energy 15, 916–929 (2021). https://doi.org/10.1007/s11708-021-0757-9
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DOI: https://doi.org/10.1007/s11708-021-0757-9