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Neutron energy

Thermal neutron absorption cross section. Simply designated cross section, it represents the ease with which a given nuclide can absorb a thermal neutron (energy less than or equal to 0.025 eV) and become a different nuclide. The cross section is given here in units of barns (1 barn = 10 cm ). If the mode of reaction is other than ( ,y), it is so indicated. [Pg.333]

Greater detail in the treatment of neutron interaction with matter is required in modem reactor design. The neutron energy distribution is divided into groups governed by coupled space-dependent differential equations. [Pg.211]

One was a water-moderated and water-cooled pressurized reactor the other was a Hquid-metal-cooled iatermediate neutron energy reactor. A land-based prototype submafine power plant called Mark I was built and tested at the National Reactor Testing Station. Argonne National Laboratory provided scientific data and Bettis Laboratory of Westinghouse Electric Corp. suppHed engineering expertise. [Pg.223]

The neutron dose to graphite due to irradiation is commonly reported as a time integrated flux of neutrons per unit area (or fluence) referenced to a particular neutron energy. Neutron energies greater that 50 keV, 0.1 MeV, 0.18 MeV, and 1 MeV were adopted in the past and can be readily foimd in the literature. In the U.K., irradiation data are frequently reported in fluences referenced to a standard flux spectrum at a particular point in the DIDO reactor, for which the displacement rate was measured by the nickel activation [ Ni(np) t o] reaction [equivalent DIDO nickel (EDN)]. Early on, neutron irradiation doses to the graphite moderator were reported in terms of the bum-up (energy extracted) from imit mass of the adjacent nuclear fuel, i.e., MW days per adjacent tonne of fuel, or MWd/Ate. [Pg.459]

Effective half-life Average neutron energy Neutron emission rate Decay heat... [Pg.356]

Radionuclide An atom that is distinguished by its nucleus composition (number of protons, number of neutrons, energy content), atomic number, mass number, and atomic mass. [Pg.1756]

Nuclear reactors are classified by their neutron energy level (thermal or fast reactors), by their coolant (water, gas, liquid metal) and by their neutron moderator (light water, heavy water, graphite). Most existing plants are thermal reactors using pressurised (PWR) or boiling water (BWR) as a coolant and moderator PWR and BWR together represent more than 80% of the commercial nuclear reactors today, of which PWR accounts for 60% alone (Olah et al., 2006). [Pg.119]

Cf spontaneous fissions have a fast neutron energy spectrum, shown in Figure 3, with an average energy of 2.2MeV. On average, 3.76 neutrons are emitted per spontaneous fission. The neutron emission rate is 2.34 X 10 n/(s-g)... [Pg.65]

Unfortunately, energetic heavy ions require expensive, large accelerators to produce. If increased biological effectiveness were the main therapeutic benefit, with improved dose localization not a major issue, then neutron beams might be more desirable. Fig. 7 shows microdosimetric spectra for neutron beams as a function of the nominal neutron energy. [Pg.548]

Figure 7 Microdosimetric spectra in a 2-pm equivalent sphere as a function of neutron energy as noted. Figure 7 Microdosimetric spectra in a 2-pm equivalent sphere as a function of neutron energy as noted.
The equation shows that uranium-235 absorbs a neutron. After absorbing the neutron, the excited uranium nucleus splits and forms barium-141, krypton-92, and three neutrons. Energy is also produced in the reaction. This reaction is only one of a number of different ways that U-235 may split. Several hundred different isotopes have been identified when U-235 undergoes fission. [Pg.247]

Experimentally, scattering cross sections are measured as a function of the time of flight, t, of scattered neutron over a fixed distance, /. Final neutron energy, hiOy is related to (///) as... [Pg.132]

Additional interactions of neutrons with nuclei include die release of charged particles by neutron-induced nuclear disintegration, Commonly known reactions are n-p. n — d. and n—ct. In these cases, the incident neutrons may contribute part of their kinetic energy to the target nucleus to effect the disintegration. Hence, more than mere neutron capture is involved, Then, there is usually a lower threshold for the neutron energy below which the reaction fails to occur, Another important reaction involving neutrons is fission, which may occur under different conditions for eidier slow or fast neutrons with appropriate fissionable material. [Pg.1068]

Epithermal neutrons, or neutrons having energies just above those of thermal neutrons the epithermal neutrons energy range is between a few hundredths eV and about 100 eV. [Pg.1069]


See other pages where Neutron energy is mentioned: [Pg.210]    [Pg.211]    [Pg.5]    [Pg.122]    [Pg.401]    [Pg.431]    [Pg.458]    [Pg.863]    [Pg.874]    [Pg.9]    [Pg.142]    [Pg.144]    [Pg.422]    [Pg.452]    [Pg.479]    [Pg.480]    [Pg.38]    [Pg.127]    [Pg.81]    [Pg.9]    [Pg.332]    [Pg.61]    [Pg.62]    [Pg.62]    [Pg.62]    [Pg.63]    [Pg.66]    [Pg.66]    [Pg.72]    [Pg.353]    [Pg.539]    [Pg.1068]    [Pg.1068]    [Pg.1095]    [Pg.274]   
See also in sourсe #XX -- [ Pg.44 ]




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Bombardment of nuclei by high-energy a-particles and neutrons

Characteristic energy, neutron interaction

Energy of neutron

High-energy fission neutrons

High-energy neutrons

Mean neutron energy

Measurement of a Neutron Energy Spectrum by Proton Recoil

Neutron Energy Measurement with a Crystal Spectrometer

Neutron Kinetic energy

Neutron binding energy

Neutron continued energy dependence

Neutron energy gain

Neutron energy loss

Neutron energy spectrum

Neutron fast’/high-energy, bombardment

Neutron high-energy, bombardment

Neutron separation energy

Neutrons energy shells

Neutrons resonance energy

Reactor neutron energy spectrum

Thermal neutrons energy

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