A reactor operates at a thermal flux for long enough that its poisoning has reached…

PHYSICS · Multi-part · Fermi University Physics · Nuclear Physics · Fission, fusion and nuclear energy · Fission, fusion and nuclear energy

The Nucleus Resolved, Ch The reactor as a field equation: diffusion, criticality, feedback and burn-up

Problem

A reactor operates at a thermal flux ϕ=2.0×1013 cm−2 s−1\phi = 2.0\times10^{13}\,\mathrm{cm^{-2}\,s^{-1}} for long enough that its 135Xe^{135}\mathrm{Xe} poisoning has reached equilibrium. The equilibrium xenon reactivity is ρXeeq=−ρmax⁡ ϕϕ+ϕ0,\rho_{Xe}^{\rm eq} = -\rho_{\max}\,\frac{\phi}{\phi + \phi_0}, where ρmax⁡=2730 pcm\rho_{\max} = 2730\,\mathrm{pcm} is the saturation worth reached at very high flux and ϕ0=λXe/σXe=7.9×1012 cm−2 s−1\phi_0 = \lambda_{Xe}/\sigma_{Xe} = 7.9\times10^{12}\,\mathrm{cm^{-2}\,s^{-1}}. After shutdown the xenon concentration continues to rise for a time, peaking, at this flux, at about 1.541.54 times its equilibrium worth roughly 7.4 h7.4\,\mathrm{h} later. ((a)) Find the equilibrium xenon worth at this flux. ((b)) Find the peak xenon worth after shutdown. ((c)) The control system can supply at most 2500 pcm2500\,\mathrm{pcm} of excess reactivity to override poisoning. Decide whether the reactor can be restarted at the moment of the xenon peak.

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