Six factor formula

Formula used to calculate nuclear chain reaction growth rate

The six-factor formula is used in nuclear engineering to determine the multiplication of a nuclear chain reaction in a non-infinite medium.

Six-factor formula: k = η f p ε P F N L P T N L = k P F N L P T N L {\displaystyle k=\eta fp\varepsilon P_{FNL}P_{TNL}=k_{\infty }P_{FNL}P_{TNL}} [1]
Symbol Name Meaning Formula Typical thermal reactor value
η {\displaystyle \eta } Thermal fission factor (eta) neutrons produced from fission/absorption in fuel isotope η = ν σ f F σ a F {\displaystyle \eta ={\frac {\nu \sigma _{f}^{F}}{\sigma _{a}^{F}}}} 1.65
f {\displaystyle f} Thermal utilization factor neutrons absorbed by the fuel isotope/neutrons absorbed anywhere f = Σ a F Σ a {\displaystyle f={\frac {\Sigma _{a}^{F}}{\Sigma _{a}}}} 0.71
p {\displaystyle p} Resonance escape probability fission neutrons slowed to thermal energies without absorption/total fission neutrons p e x p ( i = 1 N N i I r , A , i ( ξ ¯ Σ p ) m o d ) {\displaystyle p\approx \mathrm {exp} \left(-{\frac {\sum \limits _{i=1}^{N}N_{i}I_{r,A,i}}{\left({\overline {\xi }}\Sigma _{p}\right)_{mod}}}\right)} 0.87
ε {\displaystyle \varepsilon } Fast fission factor (epsilon) total number of fission neutrons/number of fission neutrons from just thermal fissions ε 1 + 1 p p u f ν f P F A F f ν t P T A F P T N L {\displaystyle \varepsilon \approx 1+{\frac {1-p}{p}}{\frac {u_{f}\nu _{f}P_{FAF}}{f\nu _{t}P_{TAF}P_{TNL}}}} 1.02
P F N L {\displaystyle P_{FNL}} Fast non-leakage probability number of fast neutrons that do not leak from reactor/number of fast neutrons produced by all fissions P F N L e x p ( B g 2 τ t h ) {\displaystyle P_{FNL}\approx \mathrm {exp} \left(-{B_{g}}^{2}\tau _{th}\right)} 0.97
P T N L {\displaystyle P_{TNL}} Thermal non-leakage probability number of thermal neutrons that do not leak from reactor/number of thermal neutrons produced by all fissions P T N L 1 1 + L t h 2 B g 2 {\displaystyle P_{TNL}\approx {\frac {1}{1+{L_{th}}^{2}{B_{g}}^{2}}}} 0.99

The symbols are defined as:[2]

  • ν {\displaystyle \nu } , ν f {\displaystyle \nu _{f}} and ν t {\displaystyle \nu _{t}} are the average number of neutrons produced per fission in the medium (2.43 for uranium-235).
  • σ f F {\displaystyle \sigma _{f}^{F}} and σ a F {\displaystyle \sigma _{a}^{F}} are the microscopic fission and absorption cross sections for fuel, respectively.
  • Σ a F {\displaystyle \Sigma _{a}^{F}} and Σ a {\displaystyle \Sigma _{a}} are the macroscopic absorption cross sections in fuel and in total, respectively.
  • N i {\displaystyle N_{i}} is the number density of atoms of a specific nuclide.
  • I r , A , i {\displaystyle I_{r,A,i}} is the resonance integral for absorption of a specific nuclide.
    • I r , A , i = E t h E 0 d E Σ p m o d Σ t ( E ) σ a i ( E ) E {\displaystyle I_{r,A,i}=\int _{E_{th}}^{E_{0}}dE'{\frac {\Sigma _{p}^{mod}}{\Sigma _{t}(E')}}{\frac {\sigma _{a}^{i}(E')}{E'}}} .
  • ξ ¯ {\displaystyle {\overline {\xi }}} is the average lethargy gain per scattering event.
    • Lethargy is defined as decrease in neutron energy.
  • u f {\displaystyle u_{f}} (fast utilization) is the probability that a fast neutron is absorbed in fuel.
  • P F A F {\displaystyle P_{FAF}} is the probability that a fast neutron absorption in fuel causes fission.
  • P T A F {\displaystyle P_{TAF}} is the probability that a thermal neutron absorption in fuel causes fission.
  • B g 2 {\displaystyle {B_{g}}^{2}} is the geometric buckling.
  • L t h 2 {\displaystyle {L_{th}}^{2}} is the diffusion length of thermal neutrons.
    • L t h 2 = D Σ a , t h {\displaystyle {L_{th}}^{2}={\frac {D}{\Sigma _{a,th}}}} .
  • τ t h {\displaystyle \tau _{th}} is the age to thermal.
    • τ = E t h E d E 1 E D ( E ) ξ ¯ [ D ( E ) B g 2 + Σ t ( E ) ] {\displaystyle \tau =\int _{E_{th}}^{E'}dE''{\frac {1}{E''}}{\frac {D(E'')}{{\overline {\xi }}\left[D(E''){B_{g}}^{2}+\Sigma _{t}(E')\right]}}} .
    • τ t h {\displaystyle \tau _{th}} is the evaluation of τ {\displaystyle \tau } where E {\displaystyle E'} is the energy of the neutron at birth.

Multiplication

The multiplication factor, k, is defined as (see nuclear chain reaction):

k = number of neutrons in one generation/number of neutrons in preceding generation
  • If k is greater than 1, the chain reaction is supercritical, and the neutron population will grow exponentially.
  • If k is less than 1, the chain reaction is subcritical, and the neutron population will exponentially decay.
  • If k = 1, the chain reaction is critical and the neutron population will remain constant.

See also

  • Critical mass
  • Nuclear chain reaction
  • Nuclear reactor
  • Four factor formula

References

  1. ^ Duderstadt, James; Hamilton, Louis (1976). Nuclear Reactor Analysis. John Wiley & Sons, Inc. ISBN 0-471-22363-8.
  2. ^ Adams, Marvin L. (2009). Introduction to Nuclear Reactor Theory. Texas A&M University.