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Modified beam theory

ASTM round-robin testing [137] has shown that the modified beam theory (MBT) method (Eq. 25) yielded the most conservative values of Gjj.. Accordingly this method is recommended. [Pg.565]

Transition state theory, especially with its recent developments, has proved a very powerful tool, vastly superior to collision theory. It has only recently been challenged by modem advances in molecular beams and molecular dynamics which look at the microscopic details of a collision, and which can be regarded as a modified collision theory. These developments along with computer techniques, and modem experimental advances in spectroscopy and lasers along with fast reaction techniques, are now revolutionizing the science of reaction rates. [Pg.4]

Modified collision theory along with molecular beam studies has greatly expanded the knowledge of reaction at the microscopic level for many simple elementary reactions. [Pg.122]

This may be determined theoretically over the whole particle size refractive index domain using Mie theory or, over limited ranges, with modified theories. Other interactions between the particles and the incident radiation, such as state of polarization, light flux at a fixed angle to the direction of the incident beam and angular spectra can be used for particle size determination. [Pg.532]

From this expression, it is seen that the temporal properties of the incident radiation field depend upon the coherence time Atg and the pulse duration AT. It must be pointed out that the physical nature of these times is essentially different. For a given source, At is imposed by the uncertainty principle of quantum theory, whereas AT corresponds to a classical statistical probability distribution, which can in principle be modified by the experimenter. In particular, if one reduces this classical uncertainty" sufficiently, the time resolution conditions can be improved so as to have the lowest possible resolution time given by the quantal uncertainty" value At. This corresponds to the minimum time uncertainty situation, for which one has S(fo) (to) and therefore p to) a(to)-The spectral properties of the incident beam are best described by... [Pg.303]


See other pages where Modified beam theory is mentioned: [Pg.79]    [Pg.375]    [Pg.520]    [Pg.563]    [Pg.567]    [Pg.366]    [Pg.79]    [Pg.375]    [Pg.520]    [Pg.563]    [Pg.567]    [Pg.366]    [Pg.100]    [Pg.175]    [Pg.134]    [Pg.184]    [Pg.206]    [Pg.331]    [Pg.235]    [Pg.112]    [Pg.605]    [Pg.78]    [Pg.119]    [Pg.23]    [Pg.16]    [Pg.119]    [Pg.206]    [Pg.21]    [Pg.58]    [Pg.904]    [Pg.210]    [Pg.702]    [Pg.160]    [Pg.58]    [Pg.2]    [Pg.3]    [Pg.4]    [Pg.31]    [Pg.358]    [Pg.485]    [Pg.186]    [Pg.712]    [Pg.91]    [Pg.352]    [Pg.335]    [Pg.388]   
See also in sourсe #XX -- [ Pg.563 ]




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Beam theory

Modified beam theory method

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