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Exponential averaging, equilibrium phase

Figure 5. The time dependence of the normalized radius of gyration Rg t) and the fraction of unfolded molecules P (t) for sequence A at T = 0.947/-. Data are averaged over 100 [for Rg t) ] and 600 [for Pu t)] trajectories. P t) decays exponentially with the time scale X/ = 2.07x 10 MCS. The approach of Rg t)) to equilibrium is biexponential with the times scales 0.083x 10 MCS and 0.698 x 10 MCS. The first time scale is due to extremely rapid burst-phase partial collapse. The second time scale, which is associated with the eollapse time x, corresponds to the final compaction. The ratio x//xc is approximately 3.0. Figure 5. The time dependence of the normalized radius of gyration Rg t) and the fraction of unfolded molecules P (t) for sequence A at T = 0.947/-. Data are averaged over 100 [for Rg t) ] and 600 [for Pu t)] trajectories. P t) decays exponentially with the time scale X/ = 2.07x 10 MCS. The approach of Rg t)) to equilibrium is biexponential with the times scales 0.083x 10 MCS and 0.698 x 10 MCS. The first time scale is due to extremely rapid burst-phase partial collapse. The second time scale, which is associated with the eollapse time x, corresponds to the final compaction. The ratio x//xc is approximately 3.0.

See other pages where Exponential averaging, equilibrium phase is mentioned: [Pg.299]    [Pg.94]    [Pg.93]    [Pg.538]    [Pg.724]    [Pg.247]    [Pg.504]    [Pg.673]    [Pg.3149]    [Pg.670]    [Pg.145]    [Pg.52]   


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