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Langevin equation rotational dynamics

Here (Oe and co are delivered by the corresponding Langevin equations of the theory of the rotational Brownian motion. In order to obtain these equations, one must include in the dynamic equations (4.308) and (4.310) the random thermal torques. We do that in the following way ... [Pg.549]

Classic Brownian motion has been widely applied in the past to the interpretation of experiments sensitive to rotational dynamics. ESR and NMR measurements of T and Tj for small paramagnetic probes have been interpreted on the basis of a simple Debye model, in which the rotating solute is considered a rigid Brownian rotator, sueh that the time scale of the rotational motion is much slower than that of the angular momentum relaxation and of any other degree of freedom in the liquid system. It is usually accepted that a fairly accurate description of the molecular dynamics is given by a Smoluchowski equation (or the equivalent Langevin equation), that can be solved analytically in the absence of external mean potentials. [Pg.90]


See other pages where Langevin equation rotational dynamics is mentioned: [Pg.438]    [Pg.181]    [Pg.117]    [Pg.328]    [Pg.364]    [Pg.243]    [Pg.296]    [Pg.152]    [Pg.196]    [Pg.43]    [Pg.193]    [Pg.2611]   
See also in sourсe #XX -- [ Pg.92 , Pg.93 ]




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