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The six-factor formula is used in [[nuclear engineering]] to determine the multiplication of a [[nuclear chain reaction]] in a non-infinite medium. The formula is<ref name=Duderstadt>{{cite book |last=Duderstadt |first=James |coauthors=Hamilton, Louis |title=Nuclear Reactor Analysis |year=1976 |publisher=John Wiley & Sons, Inc |isbn=0-471-22363-8 }}</ref>
 
<center><math>k = \eta f p \epsilon P_{FNL} P_{TNL}</math></center>
 
{| class="wikitable" border="1" cellpadding="8" cellspacing="0"
! Symbol
! Name
! Meaning
! Formula
! Typical Thermal Reactor Value
|-
|<math>\eta</math>
| Thermal Fission Factor (Eta)
| The number of fission [[neutron]]s produced per absorption in the fuel.
| <math> \eta = \frac{\nu \sigma_f^F}{\sigma_a^F} </math>
| 1.65
|-
| <math>f</math>
| The thermal utilization factor
| Probability that a neutron that gets absorbed does so in the fuel material.
| <math>f = \frac{\Sigma_a^F}{\Sigma_a} </math>
| 0.71
|-
| <math>p</math>
| The resonance escape probability
| Fraction of fission neutrons that manage to slow down from fission to thermal energies without being absorbed.
| <math>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)</math>
| 0.87
|-
| <math>\epsilon</math>
| The fast fission factor (Epsilon)
| <center><math>\tfrac{\mbox{total number of fission neutrons}}{\mbox{number of fission neutrons from just thermal fissions}}</math></center>
| <math>\epsilon \approx 1 + \frac{1-p}{p}\frac{u_f \nu_f P_{FAF}}{f \nu_t P_{TAF} P_{TNL}}</math>
| 1.02
|-|
|-
| <math>P_{FNL}</math>
| The fast non-leakage probability
| The probability that a [[fast neutron]] will not leak out of the system.
| <math>P_{FNL} \approx \mathrm{exp} \left( -{B_g}^2 \tau_{th} \right)</math>
| 0.97
|-|
|-
| <math>P_{TNL}</math>
| The thermal non-leakage probability
| The probability that a [[thermal neutron]] will not leak out of the system.
| <math>P_{TNL} \approx \frac{1}{1+{L_{th}}^2 {B_g}^2}</math>
| 0.99
|-
|}
 
The symbols are defined as:<ref name=Adams>{{cite book |last=Adams |first=Marvin L. |title=Introduction to Nuclear Reactor Theory |year=2009 |publisher=Texas A&M University}}</ref>
*<math>\nu</math>, <math>\nu_f</math> and <math>\nu_t</math> are the average number of neutrons produced per fission in the medium (2.43 for [[Uranium-235]]).
*<math>\sigma_f^F</math> and <math>\sigma_a^F</math> are the microscopic fission and absorption cross sections for fuel, respectively.
*<math>\Sigma_a^F</math> and <math>\Sigma_a</math> are the macroscopic absorption cross sections in fuel and in total, respectively.
*<math>N_i</math> is the number density of atoms of a specific [[nuclide]].
*<math>I_{r,A,i}</math> is the resonance integral for absorption of a specific [[nuclide]].
**<math>I_{r,A,i} = \int_{E_{th}}^{E_0} dE' \frac{\Sigma_p^{mod}}{\Sigma_t(E')} \frac{\sigma_a^i(E')}{E'}</math>.
*<math>\overline{\xi}</math> (often referred to as ''worm-bar'' or ''squigma-bar'') is the average lethargy gain per scattering event.
**Lethargy is defined as decrease in neutron energy.
*<math>u_f</math> (fast utilization) is the probability that a fast neutron is absorbed in fuel.
*<math>P_{FAF}</math> is the probability that a fast neutron absorption in fuel causes fission.
*<math>P_{TAF}</math> is the probability that a thermal neutron absorption in fuel causes fission.
*<math>{B_g}^2</math> is the [[Geometric and Material Buckling|geometric buckling]].
*<math>{L_{th}}^2</math> is the diffusion length of thermal neutrons.
**<math>{L_{th}}^2 = \frac{D}{\Sigma_{a,th}}</math>.
*<math>\tau_{th}</math> is the age to thermal.
**<math>\tau = \int_{E_{th}}^{E'} dE'' \frac{1}{E''} \frac{D(E'')}{\overline{\xi} \left[ D(E'') {B_g}^2 + \Sigma_t(E') \right]}</math>.
**<math>\tau_{th}</math> is the evaluation of <math>\tau</math> where <math>E'</math> is the energy of the neutron at birth.
 
==Multiplication==
The multiplication factor, k, is defined as (see [[Nuclear chain reaction]]): <center><math>k = \frac{\mbox{number of neutrons in one generation}}{\mbox{number of neutrons in preceding generation}}</math></center>
 
If k is greater than 1, the chain reaction is ''supercritical,'' and the neutron population will grow exponentially. <br />
If k is less than 1, the chain reaction is ''subcritical,'' and the neutron population will exponentially decay. <br />
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==
{{reflist}}
 
[[Category:Nuclear technology]]
[[Category:Radioactivity]]

Revision as of 02:50, 26 October 2013

The six-factor formula is used in nuclear engineering to determine the multiplication of a nuclear chain reaction in a non-infinite medium. The formula is[1]

Symbol Name Meaning Formula Typical Thermal Reactor Value
Thermal Fission Factor (Eta) The number of fission neutrons produced per absorption in the fuel. 1.65
The thermal utilization factor Probability that a neutron that gets absorbed does so in the fuel material. 0.71
The resonance escape probability Fraction of fission neutrons that manage to slow down from fission to thermal energies without being absorbed. 0.87
The fast fission factor (Epsilon)
1.02
The fast non-leakage probability The probability that a fast neutron will not leak out of the system. 0.97
The thermal non-leakage probability The probability that a thermal neutron will not leak out of the system. 0.99

The symbols are defined as:[2]

Multiplication

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

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

References

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