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Model standing wave formation

It can be seen in Figs. 1.15a and b that for the model ultrathin organic film at the air-Si and water-Si interfaces aU components of the MSEEs within this film for all angles of incidence are weakened relative to the incident radiation (< () = 1). Comparison of the electric field intensities in the air and water environments reveals that the MSEF magnitudes within the film, (El), increase as the optical density of the surroundings ( i) increases. Deviation of the values of (El) from unity and their dependence on the optical parameters of the medium are due to the formation of interference patterns (standing waves) in... [Pg.50]

The rules presented operate not only in many musical instruments and the formation of standing waves in them (in the resonator of a guitar, for instance) but are also used in models of an ideal black body, in quantum mechanics, in physics of soUd-state properties, etc. All of these are discussed in other sections of the book. [Pg.160]

To simulate the pattern formation observed in our experiments, we employ a model of the BZ reaction (21). We add a global linear feedback term to account for the bromide ion production that results from the actinic illumination, vqf = naxC av ss% where q> is the quantum yield. The results of our simulations mimic those of the experiments. Bulk oscillations and travelling waves are observed in die model for smaller values of g. At higher g values, standing, irregular and localized clusters are observed in the same sequence and with the same patterns of hysteresis as in the experiments... [Pg.114]


See other pages where Model standing wave formation is mentioned: [Pg.1321]    [Pg.308]    [Pg.27]    [Pg.141]    [Pg.503]    [Pg.171]   
See also in sourсe #XX -- [ Pg.393 ]




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