Latest revision as of 13:07, 12 August 2013

Neutron Emission

@@ Line 1: / Line 1: @@
-=Neutron energy: types and spectra=
+= Neutron Emission=
-Neutron are classified into four types depending on their energy, each type has energy range which may change from one reference to another. The following table shows the types of neutrons, their energy range, and common detective materials.
+[[Neutron Emission]]
-{| border="1" cellpadding="4"
-|-
-| Neutron Type || Energy Range || Common detective material(s)
-|-
-|Cold Neutrons || || He-3
-|-
-|Thermal Neutrons || || Be-4, Li-6
-|-
-|Epithermal Neutrons || ||
-|-
-|Fast Neutrons        || || U-238, Th-232
-|}
-== Neutron Emission==
-== Induced Neutron Fission of U233 (U-238 or Th-232)===
-The cross section is defined by the following equation :<ref name="Ahmed"/>
-<math> \sigma(E) = \int \frac{d\sigma}{d\Omega} . d\Omega </math>
-where
-<math> \frac{d\sigma}{d\Omega} = \frac{1}{\Phi}\frac{dN}{d\Omega} </math>
-Where '''<math> \Phi </math>''' is the number incident particle  per uni area per unit time, '''dN''' is the average number of particles per unit time that interacted per unit solid angle, and '''<math>\Omega</math>''' is the solid angle.
-Since the cross section has an area unit (barn), some authors define this quantity as the area to which the particle is exposed to make an interaction. <ref name="Ahmed">Syed Ahmed, Physics and Engineering of Radiation Detection (Academic Press 2007) </ref> The cross section values are represented as a function of energy that gives the value of the cross section for each energy value and shows the resonance peaks.  A theoretical description of the neutron fission cross section curve is not available, but statistically it is possible to evaluate the parameters for an assumption that describes part of the cross section curve within a certain error.<ref name="Hyde"/>
-Neutron fission is one of the interactions that commonly takes place spontaneously or under certain experimental conditions. An incident neutron depositing sufficient energy in a nucleus to  enable the nucleus to overcome the Coulomb barrier will cause the nucleus to split into fragment ligher nuclei (fragments) and particles. The new products interact with the surrounding medium depending on their energy and the type of the medium that contains them.
-Both  U-238 and Th-232 are members of the actinides group. They are characterized by relatively high neutron fission cross sections for fast neutrons with  fission thresholds above the thermal neutron energy. The fission reaction in both elements is expected to eject 1-2 neutrons when the incident neutron energy is between 5-10 MeV as shown in Fig.9 and Fig.10.
-{| border="1" cellpadding="4"
-|-
-|[[ File:ENDF_GEAN4_U238_fxsection.png |250 px]] ||[[File: Th_232_reference.png|250 px]]
-|-
-|Fig.9 U 238  fission cross section || Fig.10 Th 232  fission cross section <ref name="endf_Th_232_JEFF1.3">http://www.nndc.bnl.gov/exfor/servlet/E4sMakeE4 </ref>
-|}

Difference between revisions of "Induced Neutron Fission Fragment"

Latest revision as of 13:07, 12 August 2013

Neutron Emission

Navigation menu

Search