Startup neutron source

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RBMK type reactor control rod layout; blue=startup neutron sources (12), yellow=shortened control rods from the reactor bottom (32), grey=pressure tubes (1661), green=control rods (167), red=automatic control rods (12)

Startup neutron source is a neutron source used for stable and reliable initiation of nuclear chain reaction in nuclear reactors, when they are loaded with fresh nuclear fuel, whose neutron flux from spontaneous fission is insufficient for a reliable startup, or after prolonged shutdown periods. Neutron sources ensure a constant minimal population of neutrons in the reactor core, sufficient for a smooth startup. Without them, the reactor could suffer fast power excursions during startup from state with too few self-generated neutrons (new core or after extended shutdown).

The startup sources are typically inserted in regularly spaced positions inside the reactor core, in place of some of the fuel rods.

The sources are important for safe reactor startup. The spontaneous fission and cosmic rays serve as weak neutron sources, but these are too weak for the reactor instrumentation to detect; relying on them could lead to a "blind" start, which is a potentially unsafe condition.[1] The sources are therefore positioned so the neutron flux they produce is always detectable by the reactor monitoring instruments. When the reactor is in shutdown state, the neutron sources serve to provide signals for neutron detectors monitoring the reactor, to ensure they are operable.[2] The equilibrium level of neutron flux in a subcritical reactor is dependent on the neutron source strength; a certain minimum level of source activity therefore has to be ensured in order to maintain control over the reactor when in strongly subcritical state, namely during startups.[3]

The sources can be of two types:[4]

When plutonium-238/beryllium primary sources are utilized, they can be either affixed to control rods which are removed from the reactor when it is powered, or clad in a cadmium alloy, which is opaque to thermal neutrons (reducing transmutation of the plutonium-238 by neutron capture) but transparent to fast neutrons produced by the source.[2]

  • Secondary sources, originally inert, become radioactive and neutron-producing only after neutron activation in the reactor. Due to this, they tend to be less expensive. Exposure to thermal neutrons also serves to maintain the source activity (the radioactive isotopes are both burned and generated in neutron flux).

The chain reaction in the first critical reactor, CP-1, was initiated by a radium-beryllium neutron source. Similarly, in modern reactors (after startup), delayed neutron emission from fission products suffices to sustain the amplification reaction while yielding controllable growth times. In comparison, a bomb is based on immediate neutrons and grows exponentially in nanoseconds.


  1. ^ Atomic Energy of Canada (1997). Canada enters the nuclear age: a technical history of Atomic Energy of Canada Limited. McGill-Queen's Press - MQUP. p. 224. ISBN 0-7735-1601-8.
  2. ^ a b U.S. Patent 4,208,247 Neutron source
  3. ^ "Microsoft Word - lecture25.doc" (PDF). Archived from the original (PDF) on June 29, 2011. Retrieved 2010-03-28.
  4. ^ Ken Kok (2009). Nuclear Engineering Handbook. CRC Press. p. 27. ISBN 978-1-4200-5390-6.
  5. ^ a b Integrated Publishing. "Neutron Sources Summary". Retrieved 2010-03-28. CS1 maint: discouraged parameter (link)
  6. ^ Karl-Heinz Neeb (1997). The radiochemistry of nuclear power plants with light water reactors. Walter de Gruyter. p. 147. ISBN 3-11-013242-7.
  7. ^ "Memorandum from Raymond L. Murray to Dr. Clifford K. Beck". Retrieved 2010-03-28. CS1 maint: discouraged parameter (link)