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Emission of charged particles

The numerator of the first term is the number of ways N white balls could appear in 6 draws, and the denominator N is the number of ways these same Ar white balls could be interchanged. (Division by N in the first term reflects the fact that the order in which any specific white ball is drawn is unimportant, since this division by Nl produces the effect of making individual white balls indistinguishable.) If the decomposition of radioactive atoms and the resultant emission of charged particles really follow the laws of chance that govern the drawing of balls from a bag, then radioactivity must be a random process. [Pg.271]

Decay, Radioactive—Transformation of the nucleus of an unstable nuclide by spontaneous emission of charged particles and/or photons (see Disintegration). [Pg.272]

NDP is a prompt nuclear analysis technique, which employs a nuclear reaction that results in emission of charged particles with a specific kinetic energy. It is one of the most powerful non-destructive techniques for depth profiling of some light elements especially for and Li, which have very high thermal neutron capture cross-sections of 3837 and 940 barn respectively. [Pg.545]

Other important competing reactions that can occur in samples, are the neutron-induced emission of charged particles, specifically (n,p), (n,ot) reactions, and fission, noted as (n,f) reaction (Molnar 2004). The most important cases are the following ... [Pg.1622]

In a sample exposed to neutrons several types of nuclear reactions may take place, depending on the energy of the neutrons and on the elements present. The probability of a particular reaction is expressed by the activation cross-section, o a, which is usually larger for the simple neutron capture (n,-y) process than for processes such as (n,p) and (n,a), involving the emission of charged particles. The most sensitive radioaetive indicators are therefore isotopie with the element to be determined. [Pg.185]

Emission of charged particles exoelectron) [11, 12] and light chemiluminescence) [13-15] during gas adsorption or reaction is generally attributed to a nonadiabatic charge transfer process. [Pg.232]

The physical effects that lead to the eventual desorption of secondary particles are not yet completely understood. Whereas the desorption of secondary neutrals from elemental targets can be described fairly well, an explanation of the emission of charged particles and. in particular, the emission of molecular species, is still being sought. Nevertheless, there is consensus that. sputtering is based primarily on the formation of a collision cascade in tbe target caused by the impinging primary ion 3. 4J. [Pg.210]

As he continued to study filaments in vacuum and different gas environments, he began to study the emission of charged particles from hot filaments (thermionic emission). He was one of the first scientists to work with plasmas and was the first to call these ionized gases by that name, because they reminded him of blood plasma. Langmuir and Tonks discovered electron density waves in plasmas that are now known as Langmuir waves. [Pg.413]


See other pages where Emission of charged particles is mentioned: [Pg.372]    [Pg.156]    [Pg.234]    [Pg.382]    [Pg.146]    [Pg.200]    [Pg.874]    [Pg.1312]    [Pg.245]    [Pg.288]    [Pg.193]    [Pg.1723]    [Pg.395]    [Pg.953]    [Pg.247]    [Pg.939]    [Pg.283]   
See also in sourсe #XX -- [ Pg.69 , Pg.146 ]




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