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Neutron disintegration

Other nuclei having higher number of protons or neutrons disintegrate by (a). [Pg.196]

Whenever a radioactive element emits a /3 particle, its daughter has a mass number that is the same as that of the parent and an atomic number that is 1 greater than that of the parent. Because electrons as such are not present in the nuclei of atoms, it is not obvious at first why the loss of a ft particle should cause an increase in atomic number. What actually happens is that a neutron disintegrates ... [Pg.402]

Baryons are held together in atomic nuclei by strong interaction and at least one further level of reduction at which protons and neutrons are separated, can be envisaged. Since a free neutron disintegrates spontaneously, ponderable matter can be considered as made up of protons, electrons and neutrinos. Each of these carry characteristic amounts of mass, charge and spin. The neutrino apparently has zero mass and charge. [Pg.246]

Atoms with the same number of protons but a different number of neutrons are called isotopes. To identify an isotope we use the symbol E, where E is the element s atomic symbol, Z is the element s atomic number (which is the number of protons), and A is the element s atomic mass number (which is the sum of the number of protons and neutrons). Although isotopes of a given element have the same chemical properties, their nuclear properties are different. The most important difference between isotopes is their stability. The nuclear configuration of a stable isotope remains constant with time. Unstable isotopes, however, spontaneously disintegrate, emitting radioactive particles as they transform into a more stable form. [Pg.642]

Three common quantitative applications of radiochemical methods of analysis are considered in this section the direct analysis of radioactive isotopes by measuring their rate of disintegration, neutron activation, and the use of radioactive isotopes as tracers in isotope dilution. [Pg.644]

Graphite will creep imder neutron irradiation and stress at temperatures where thermal creep is normally negligible. The phenomenon of irradiation creep has been widely studied because of its significance to the operation of graphite moderated fission reactors. Indeed, if irradiation induced stresses in graphite moderators could not relax via radiation creep, rapid core disintegration would result. The observed creep strain has traditionally been separated into a primary reversible component ( ,) and a secondary irreversible component (Ej), both proportional to stress and to the appropriate unirradiated elastic compliance (inverse modulus) [69]. The total irradiation-induced creep strain (ej is thus ... [Pg.468]

The products of nuclear fission reactions are radioactive and disintegrate according to their own time scales. Often disintegration leads to other radioactive products. A few of these secondary products emit neutrons that add to the pool of neutrons produced by nuclear fission. Very importantly, neutrons from nuclear fission occur before those from radioactive decay. The neutrons from nuclear fission are termed prompt. Those from radioacth e decay arc termed delayed. A nuclear bomb must function on only prompt neutrons and in so doing requires nearly 100 percent pure (or Pu) fuel. Although reactor... [Pg.864]

We can use Fig. 17.13 to predict the type of disintegration that a radioactive nuclide is likely to undergo. Nuclei that lie above the band of stability are neutron rich they have a high proportion of neutrons. These nuclei tend to decay in such a way that the final n/p ratio is closer to that found in the band of stability. For example, a l4C nucleus can reach a more stable state by ejecting a (3 particle, which reduces the n/p ratio as a result of the conversion of a neutron into a proton (Fig. 17.15) ... [Pg.824]

When Z gets big enough, no number of neutrons is enough to stabilize the nucleus. Notice in Figure 2-20 that there are no stable nuclei above bismuth, Z — 83. Some elements with higher Z are found on Earth, notably radium (Z = 88), thorium (Z = 90), and uranium (Z = 92), but all such elements are unstable and eventually disintegrate into nuclei with Z < 83. Consequently, the set of stable nuclei, those that make up the world of normal chemistry and provide the material for all terrestrial chemical reactions, is a small subset of all possible nuclei. [Pg.90]

Conversely, nuclei that contain an excess of protons undergo proton to neutron transition with the emission of a positively charged beta particle known as a positron Q8+) and with the reduction of the atomic number by one. A positron has only a very short existence, combining immediately with an electron of a nearby atom. The two particles disintegrate in the process with the emission of two gamma rays, e.g. [Pg.198]


See other pages where Neutron disintegration is mentioned: [Pg.18]    [Pg.44]    [Pg.13]    [Pg.18]    [Pg.44]    [Pg.13]    [Pg.340]    [Pg.340]    [Pg.155]    [Pg.156]    [Pg.1287]    [Pg.476]    [Pg.461]    [Pg.792]    [Pg.860]    [Pg.865]    [Pg.415]    [Pg.18]    [Pg.23]    [Pg.959]    [Pg.177]    [Pg.113]    [Pg.57]    [Pg.663]    [Pg.25]    [Pg.450]    [Pg.482]    [Pg.1663]    [Pg.6]    [Pg.1638]    [Pg.1639]    [Pg.11]    [Pg.12]    [Pg.14]    [Pg.128]    [Pg.179]    [Pg.226]    [Pg.235]    [Pg.15]    [Pg.272]    [Pg.66]   
See also in sourсe #XX -- [ Pg.402 ]




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