“Neutron flux”的意思、由来-开放百科全书

The neutron flux is a scalar quantity used in nuclear physics and nuclear reactor physics. It is the total length travelled by all free neutrons per unit time and volume.^[1] Equivalently, it can be defined as the number of neutrons travelling through a small sphere of radius

in a time interval, divided by

(the cross section of the sphere) and by the time interval.^[2] The usual unit is cm⁻²s⁻¹ (neutrons per centimeter squared per second).

The neutron fluence is defined as the neutron flux integrated over a certain time period, so its usual unit is cm⁻² (neutrons per centimeter squared).

Natural neutron flux

Neutron flux in asymptotic giant branch stars and in supernovae is responsible for most of the natural nucleosynthesis producing elements heavier than iron. In stars there is a relatively low neutron flux on the order of 10⁵ to 10¹¹ cm⁻² s⁻¹, resulting in nucleosynthesis by the s-process (slow-neutron-capture-process). By contrast, after a core-collapse supernova, there is an extremely high neutron flux, on the order of 10²² cm⁻² s⁻¹, resulting in nucleosynthesis by the r-process (rapid-neutron-capture-process).

Atmospheric neutron flux, apparently from thunderstorms, can reach levels of 3·10⁻² to 9·10⁺¹ cm⁻² s⁻¹.^[3]^[4] However, recent results^[5] (considered invalid by the original investigators^[6]) obtained with unshielded scintillation neutron detectors show a decrease in the neutron flux during thunderstorms. Recent research appears to support lightning generating 10¹³ - 10¹⁵ neutrons per discharge via photonuclear processes.^[7]

Artificial neutron flux

Artificial neutron flux refers to neutron flux which is man-made, either as byproducts from weapons or nuclear energy production or for a specific application such as from a research reactor or by spallation. A flow of neutrons is often used to initiate the fission of unstable large nuclei. The additional neutron(s) may cause the nucleus to become unstable, causing it to decay (split) to form more stable products. This effect is essential in fission reactors and nuclear weapons.

Within a nuclear fission reactor, the neutron flux is the primary quantity measured to control the reaction inside. The flux shape is the term applied to the density or relative strength of the flux as it moves around the reactor. Typically the strongest neutron flux occurs in the middle of the reactor core, becoming lower toward the edges. The higher the neutron flux the greater the chance of a nuclear reaction occurring as there are more neutrons going through an area per unit time.

Reactor vessel wall neutron fluence

A reactor vessel of a typical nuclear power plant (PWR) endures in 40 years (32 full reactor years) of operation approximately 6.5×10¹⁹ cm⁻² (E > 1 MeV).^[8] Neutron flux causes reactor vessels to suffer from Neutron embrittlement and the steel gets activated.

See also

References

1. ^Rudi J. J. Stamm'ler, Máximo Julio Abbate, Methods of steady-state reactor physics in nuclear design. {{ISBN|978-0126633207}}
2. ^K. H. Beckurts, K. Wirtz: Neutron Physics. Springer 1964, {{ISBN|978-3-642-87616-5}}, pages 82-83
3. ^{{cite journal |last1=Gurevich |first1=A. V. |last2=Antonova |first2=V. P. |year=2012 |title=Strong Flux of Low-Energy Neutrons Produced by Thunderstorms |journal=Physical Review Letters |volume=108 |issue=12 |page= 125001|publisher=Americal Physical Society |doi=10.1103/PhysRevLett.108.125001 |bibcode = 2012PhRvL.108l5001G |pmid=22540588}}
4. ^{{cite journal |last1=Gurevich |first1=A. V. |last2=Almenova |first2=A. M. |year=2016 |title=Observations of high-energy radiation during thunderstorms at Tien-Shan |journal=Physical Review D |volume=94 |issue=2 |page= 023003|publisher=Americal Physical Society |doi=10.1103/PhysRevD.94.023003|bibcode=2016PhRvD..94b3003G }}
5. ^{{cite journal |last1=Alekseenko |first1=V. |last2=Arneodo |first2=F. |last3=Bruno |first3=G. |last4=Di Giovanni |first4=A. |last5=Fulgion |first5=W. |last6=Gromushkin |first6=D. |last7=Shchegolev |first7=O. |last8=Stenkin |first8=Yu. |last9=Stepanov |first9=V. |last10=Sulakov |first10=V. |last11=Yashin |first11=I. |year=2015 |title=Decrease of Atmospheric Neutron Counts Observed during Thunderstorms |journal=Physical Review Letters |volume=114 |issue=12 |pages= |publisher=Americal Physical Society |doi=10.1103/PhysRevLett.114.125003 |bibcode = 2015PhRvL.114l5003A}}
6. ^{{cite journal |last1=Gurevich |first1=A. V. |last2=Ptitsyn |first2=M. O. |year=2015 |title=Comment on "Decrease of Atmospheric Neutron Counts Observed during Thunderstorms" |journal=Physical Review Letters |volume=115 |issue=12 |page= 179501|publisher=Americal Physical Society |doi=10.1103/PhysRevLett.115.179501|bibcode=2015PhRvL.115q9501G }}
7. ^{{cite journal |last1=Köhn |first1=Christoph |last2=Diniz |first2=Gabriel |last3=Harakeh |first3=GMushin |year=2017 |title=Production mechanisms of leptons, photons, and hadrons and their possible feedback close to lightning leaders|journal=Journal of Geophysical Research: Atmospheres |volume=122 |issue=2 |pages= 1366|publisher=Americal Geophysical Union |doi=10.1002/2016JD025445 |bibcode =2017JGRD..122.1365K |pmid= |pmc=5349290 }}
8. ^Nuclear Power Plant Borssele Reactor Pressure Vessel Safety Assessment, p. 29, 5.6 Neutron Fluence Calculation.